FIELD OF THE INVENTION
[0001] The present invention generally relates to switchable electrochromic devices, such
as architectural windows, capable of coordinated switching over substantially their
entire area or a selected subregion of their entire area. More particularly, and in
one preferred embodiment, the present invention is directed to switchable electrochromic
multi-layer devices, particularly large area rectangular windows for architectural
applications that switch in a spatially coordinated manner over substantially their
entire area or a selected subregion of their entire area; optionally these are of
non-uniform shape, optionally they switch synchronously,
i.e., uniformly, over substantially their entire area or a selected subregion of their
entire area, or in a coordinated but nonsynchronous manner (
e.g., from side-to-side, or top-to-bottom) from a first optical state,
e.g., a transparent state, to a second optical state,
e.g., a reflective or colored state.
BACKGROUND OF THE INVENTION
[0002] Commercial switchable glazing devices are well known for use as mirrors in motor
vehicles, automotive windows, aircraft window assemblies, sunroofs, skylights, architectural
windows. Such devices may comprise, for example, inorganic electrochromic devices,
organic electrochromic devices, switchable mirrors, and hybrids of these having two
conducting layers with one or more active layers between the conducting layers. When
a voltage is applied across these conducting layers the optical properties of a layer
or layers in between change. Such optical property changes are typically a modulation
of the transmissivity of the visible or the solar subportion of the electromagnetic
spectrum. For convenience, the two optical states will be referred to as a lightened
state and a darkened state in the following discussion, but it should be understood
that these are merely examples and relative terms (
i.e., one of the two states is "lighter" or more transmissive than the other state) and
that there could be a set of lightened and darkened states between the extremes that
are attainable for a specific electrochromic device; for example, it is feasible to
switch between intermediate lightened and darkened states in such a set.
[0003] Switching between a lightened and a darkened state in relatively small electrochromic
devices such as an electrochromic rear-view mirror assembly is typically quick and
uniform, whereas switching between the lightened and darkened state in a large area
electrochromic device can be slow and spatially non-uniform. Gradual, non-uniform
coloring or switching is a common problem associated with large area electrochromic
devices. This problem, commonly referred to as the "iris effect," is typically the
result of the voltage drop through the transparent conductive coatings providing electrical
contact to one side or both sides of the device. For example, when a voltage is initially
applied to the device, the potential is typically the greatest in the vicinity of
the edge of the device (where the voltage is applied) and the least at the center
of the device; as a result, there may be a significant difference between the transmissivity
near the edge of the device and the transmissivity at the center of the device. Over
time, however, the difference in applied voltage between the center and edge decreases
and, as a result, the difference in transmissivity at the center and edge of the device
decreases. In such circumstances, the electrochromic medium will typically display
non-uniform transmissivity by initially changing the transmissivity of the device
in the vicinity of the applied potential, with the transmissivity gradually and progressively
changing towards the center of the device as the switching progresses. While the iris
effect is most commonly observed in relatively large devices, it also can be present
in smaller devices that have correspondingly higher resistivity conducting layers.
SUMMARY OF THE INVENTION
[0004] Among the various aspects of the present invention is the provision of relatively
large-area electrochromic multi-layer devices capable of coordinated switching and
coloring, across substantially its entire area that can be easily manufactured.
[0005] Briefly, therefore, the present invention is directed to a multi-layer device comprising
a first substrate and a first electrically conductive layer on a surface thereof.
The first electrically conductive layer is transmissive to electromagnetic radiation
having a wavelength in the range of infrared to ultraviolet and has a sheet resistance,
R
s, to the flow of electrical current through the first electrically conductive layer
that varies as a function of position in the first electrically conductive layer wherein
the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least 2.
[0006] Another aspect of the present invention is a multi-layer device comprising a first
substrate and a first electrically conductive layer on a surface thereof. The first
electrically conductive layer has a spatially varying sheet resistance, R
s, to the flow of electrical current through the first electrically conductive layer
that varies as a function of position in the first electrically conductive layer wherein
the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 1.25.
[0007] Another aspect of the present invention is a multi-layer device comprising a first
substrate, a first electrically conductive layer on a surface of that substrate, and
a first electrode layer on a surface of the first electrically conductive layer. The
first electrically conductive layer has a spatially varying sheet resistance, R
s, that varies as a function of position in the first electrically conductive layer
wherein the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 1.25.
[0008] Another aspect of the present invention is a multi-layer device comprising a first
substrate and a first electrically conductive layer on a surface of the substrate.
The first electrically conductive layer has a spatially varying sheet resistance,
R
s, that varies as a function of position in the first electrically conductive layer
wherein a contour map of the sheet resistance, R
s, as a function of position within the first electrically conductive layer contains
a set of isoresistance lines and a set of resistance gradient lines normal to the
isoresistance lines. The sheet resistance along a gradient line in the set generally
increases, generally decreases, generally increases until it reaches a maximum and
then generally decreases, or generally decreases until it reaches a minimum and then
generally increases. In one embodiment, for example, the gradient in sheet resistance
is a constant. By way of further example, in one embodiment, the gradient in sheet
resistance is a constant and the substrate is rectangular in shape.
[0009] Another aspect of the present invention is a multi-layer device comprising a first
substrate, a first electrically conductive layer on a surface of the substrate, and
a first electrode layer on a surface of the first electrically conductive layer. The
first electrically conductive layer has a spatially varying sheet resistance, R
s, that varies as a function of position in the first electrically conductive layer
wherein a contour map of the sheet resistance, R
s, as a function of position within the first electrically conductive layer contains
a set of isoresistance lines and a set of resistance gradient lines normal to the
isoresistance lines. The sheet resistance along a gradient line in the set generally
increases, generally decreases, generally increases until it reaches a maximum and
then generally decreases, or generally decreases until it reaches a minimum and then
generally increases. In one embodiment, for example, the gradient in sheet resistance
is a constant. By way of further example, in one embodiment, the gradient in sheet
resistance is a constant and the substrate is rectangular in shape
[0010] Another aspect of the present invention is an electrochromic multi-layer device comprising
an electrochromic layer between and in electrical contact with a first and a second
electrically conductive layer. The first and/or second electrically conductive layers
have a spatially varying sheet resistance, R
s, that varies as a function of position in the first and/or second electrically conductive
layer(s) wherein a contour map of the sheet resistance, R
s, as a function of position within the first and/or second electrically conductive
layer(s) contains a set of isoresistance lines and a set of resistance gradient lines
normal to the isoresistance lines. The sheet resistance along a gradient line in the
first and/or second electrically conductive layer(s) generally increase(s), generally
decrease(s), generally increase(s) until it reaches a maximum and then generally decrease(s),
or generally decrease(s) until it reaches a minimum and then generally increase(s)..
In one embodiment, for example, the gradient in sheet resistance is a constant. By
way of further example, in one embodiment, the gradient in sheet resistance is a constant
and the substrate is rectangular in shape
[0011] A further aspect of the present invention is an electrochromic device comprising
a first substrate, a first electrically conductive layer, a first electrode layer,
a second electrically conductive layer and a second substrate. The first and second
electrically conductive layers each have a sheet resistance, R
s, to the flow of electrical current through the first and second electrically conductive
layers that varies as a function of position in the first and second electrically
conductive layers, respectively, wherein the ratio of the value of maximum sheet resistance,
R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least 2 and the ratio of the value
of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer is at least 2. The first substrate and
the first electrically conductive layer are transmissive to electromagnetic radiation
having a wavelength in the range of infrared to ultraviolet. For example, in one embodiment
the first substrate and the first electrically conductive layer are transparent to
electromagnetic radiation having a wavelength in the range of infrared to ultraviolet.
[0012] A further aspect of the present invention is a process for modulating the transmissivity
of an electrochromic multi-layer device, the multi-layer device comprising an electrochromic
layer between and in electrical contact with a first and a second electrically conductive
layer. The process comprises applying a voltage pulse between the first and second
electrically conductive layers, the voltage pulse having a magnitude of at least about
2 volts. The voltage pulse induces the electrochromic layer to switch from a first
to a second optical state wherein the first or second optical state has a greater
transmissivity to electromagnetic radiation having a wavelength in the range of ultraviolet
to infrared wavelengths relative to the other optical state, and the second optical
state persists at least 1 second after the pulse and in the absence of a voltage applied
between the electrically conductive layers.
[0013] A further aspect of the present invention is a process for the preparation of a multi-layer
device, the process comprises forming a first electrically conductive layer on a surface
of a first substrate. The first electrically conductive layer comprises a transparent
conductor and has a spatially varying sheet resistance, R
s, to the flow of electrical current through the first electrically conductive layer
that varies as a function of position in the first electrically conductive layer wherein
the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 1.25
[0014] A further aspect of the present invention is a process for the preparation of a multi-layer
device. The process comprises forming a multilayer structure comprising an electrochromic
layer, an electrically conductive layer and a substrate, the electrically conductive
layer being between the first electrode layer and the substrate. The first electrically
conductive layer has a spatially varying sheet resistance, R
s, to the flow of electrical current through the first electrically conductive layer
that varies as a function of position in the first electrically conductive layer wherein
the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 1.25
[0015] A further aspect of the present invention is directed to a process for the preparation
of a multi-layer device. The process comprises forming a multi-layer layer structure
comprising an electrochromic layer between and in electrical contact with a first
and a second electrically conductive layer. The first and/or the second electrically
conductive layer has a spatially varying sheet resistance, R
s, to the flow of electrical current through the first and/or the second electrically
conductive layer that varies as a function of position in the first and/or the second
electrically conductive layer, respectively, wherein the ratio of the value of maximum
sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first and/or the second electrically conductive layer is at least about 1.25,
respectively.
[0016] Other objects and features will be in part apparent and in part pointed out hereinafter.
BRIEF DESCRIPTION OF THE DRAWINGS
[0017]
FIG.1 is a schematic cross-section of a multi-layer electrochromic device of the present
invention.
FIG. 2A- 2E is a series of contour maps of the sheet resistance, Rs, in the first and/or second electrically conductive layer as a function of position
(two-dimensional) within the first and/or second electrically conductive layer showing
isoresistance lines (also sometimes referred to as contour lines) and resistance gradient
lines (lines perpendicular to the isoresistance lines) resulting from various alternative
arrangements of bus bars for devices having square and circular perimeters.
FIG. 3 is a schematic cross-section of an electrically conductive layer having a graded
thickness on a substrate.
FIG. 4 is a schematic cross-section of an alternative embodiment of a multi-layer
electrochromic device of the present invention.
FIG. 5 is a 1-D lumped element circuit model diagram used to simulate dynamic behavior
of an electrochromic device as described in Example 1.
FIG. 6 is plot of the voltage waveform applied to the bus bars as described in Example
1.
FIG. 7 is plot of current flowing into the device versus time as described in Example
1.
FIG. 8 is plot of the voltage across the electrochromic film at three locations (near
the edge, near the center, and between these two) as described in Example 1.
FIG. 9 is plot of the voltage waveform applied to the bus bars as described in Example
1.
FIG. 10 is plot of current flowing into the device versus time as described in Example
1.
FIG. 11 is plot of the voltage across the electrochromic film at three locations (near
the edge, near the center, and between these two) as described in Example 1.
FIG. 12 is a 1-D lumped element circuit model diagram used to simulate dynamic behavior
of an electrochromic device as described in Example 2.
FIG. 13 is plot of the voltage waveform applied to the bus bars as described in Example
1.
FIG. 14 is plot of current flowing into the device versus time as described in Example
1.
FIG. 15 is plot of the voltage across the electrochromic film at three locations (near
the edge, near the center, and between these two as described in Example 1.
FIG. 16 is a 1-D lumped element circuit model diagram used to simulate dynamic behavior
of an electrochromic device as described in Example 3.
FIG. 17 is plot of the voltage waveform applied to the bus bars as described in Example
1.
FIG. 18 is plot of current flowing into the device versus time as described in Example
1.
FIG. 19 is plot of the voltage across the electrochromic film at three locations (near
the edge, near the center, and between these two) as described in Example 1.
FIG. 20 is a schematic cross-section of an alternative embodiment of a multi-layer
electrochromic device of the present invention.
FIG. 21 is an exploded view of the multi-layer device of FIG. 1.
[0018] Corresponding reference characters indicate corresponding parts throughout the drawings.
Additionally, relative thicknesses of the layers in the different figures do not represent
the true relationship in dimensions. For example, the substrates are typically much
thicker than the other layers. The figures are drawn only for the purpose to illustrate
connection principles, not to give any dimensional information.
ABBREVIATIONS AND DEFINITIONS
[0019] The following definitions and methods are provided to better define the present invention
and to guide those of ordinary skill in the art in the practice of the present invention.
Unless otherwise noted, terms are to be understood according to conventional usage
by those of ordinary skill in the relevant art.
[0020] The term "anodic electrochromic layer" refers to an electrode layer that changes
from a more transmissive state to a less transmissive state upon the removal of ions.
[0021] The term "cathodic electrochromic layer" refers to an electrode layer that changes
from a more transmissive state to a less transmissive state upon the insertion of
ions.
[0022] The terms "conductive" and "resistive" refer to the electrical conductivity and electrical
resistivity of a material.
[0023] The term "convex polygon" refer to a simple polygon in which every internal angle
is less than or equal to 180 degrees, and every line segment between two vertices
remains inside or on the boundary of the polygon. Exemplary convex polygons include
triangles, rectangles, pentagons, hexagons,
etc., in which every internal angle is less than or equal to 180 degrees and every line
segment between two vertices remains inside or on the boundary of the polygon.
[0024] The term "electrochromic layer" refers to a layer comprising an electrochromic material.
[0025] The term "electrochromic material" refers to materials that are able to change their
optical properties, reversibly, as a result of the insertion or extraction of ions
and electrons. For example, an electrochromic material may change between a colored,
translucent state and a transparent state.
[0026] The term "electrode layer" refers to a layer capable of conducting ions as well as
electrons. The electrode layer contains a species that can be oxidized when ions are
inserted into the material and contains a species that can be reduced when ions are
extracted from the layer. This change in oxidation state of a species in the electrode
layer is responsible for the change in optical properties in the device.
[0027] The term "electrical potential," or simply "potential," refers to the voltage occurring
across a device comprising an electrode/ion conductor/electrode stack .
[0028] The term "transmissive" is used to denote transmission of electromagnetic radiation
through a material.
[0029] The term "transparent" is used to denote substantial transmission of electromagnetic
radiation through a material such that, for example, bodies situated beyond or behind
the material can be distinctly seen or imaged using appropriate image sensing technology.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0030] FIG. 1 depicts a cross-sectional structural diagram of electrochromic device 1 according
to a first embodiment of the present invention. Moving outward from the center, electrochromic
device 1 comprises an ion conductor layer 10. First electrode layer 20 is on one side
of and in contact with a first surface of ion conductor layer 10, and second electrode
layer 21 is on the other side of and in contact with a second surface of ion conductor
layer 10. In addition, at least one of first and second electrode layers 20, 21 comprises
electrochromic material; in one embodiment, first and second electrode layers 20,
21 each comprise electrochromic material. The central structure, that is, layers 20,
10, 21, is positioned between first and second electrically conductive layers 22 and
23 which, in turn, are arranged against outer substrates 24, 25. Elements 22, 20,
10, 21, and 23 are collectively referred to as an electrochromic stack 28.
[0031] Electrically conductive layer 22 is in electrical contact with one terminal of a
power supply (not shown) via bus bar 26 and electrically conductive layer 23 is in
electrical contact with the other terminal of a power supply (not shown) via bus bar
27 whereby the transmissivity of electrochromic device 10 may be changed by applying
a voltage pulse to electrically conductive layers 22 and 23. The pulse causes electrons
and ions to move between first and second electrode layers 20 and 21 and, as a result,
electrochromic material in the first and/or second electrode layer(s) change(s) optical
states, thereby switching electrochromic device 1 from a more transmissive state to
a less transmissive state, or from a less transmissive state to a more transmissive
state. In one embodiment, electrochromic device 1 is transparent before the voltage
pulse and less transmissive (
e.g., more reflective or colored) after the voltage pulse or
vice versa.
[0032] It should be understood that the reference to a transition between a less transmissive
and a more transmissive state is non-limiting and is intended to describe the entire
range of transitions attainable by electrochromic materials to the transmissivity
of electromagnetic radiation. For example, the change in transmissivity may be a change
from a first optical state to a second optical state that is (i) relatively more absorptive
(
i.e., less transmissive) than the first state, (ii) relatively less absorptive (
i.e., more transmissive) than the first state, (iii) relatively more reflective (
i.e., less transmissive) than the first state, (iv) relatively less reflective (
i.e., more transmissive) than the first state, (v) relatively more reflective and more
absorptive (
i.e., less transmissive) than the first state or (vi) relatively less reflective and
less absorptive (
i.e., more transmissive) than the first state. Additionally, the change may be between
the two extreme optical states attainable by an electrochromic device,
e.g., between a first transparent state and a second state, the second state being opaque
or reflective (mirror). Alternatively, the change may be between two optical states,
at least one of which is intermediate along the spectrum between the two extreme states
(
e.g., transparent and opaque or transparent and mirror) attainable for a specific electrochromic
device. Unless otherwise specified herein, whenever reference is made to a less transmissive
and a more transmissive, or even a bleached-colored transition, the corresponding
device or process encompasses other optical state transitions such as non-reflective-reflective,
transparent-opaque,
etc. Further, the term "bleached" refers to an optically neutral state,
e.g., uncolored, transparent or translucent. Still further, unless specified otherwise
herein, the "color" of an electrochromic transition is not limited to any particular
wavelength or range of wavelengths. As understood by those of skill in the art, the
choice of appropriate electrochromic and counter electrode materials governs the relevant
optical transition.
[0033] In general, the change in transmissivity preferably comprises a change in transmissivity
to electromagnetic radiation having a wavelength in the range of infrared to ultraviolet
radiation. For example, in one embodiment the change in transmissivity is predominately
a change in transmissivity to electromagnetic radiation in the infrared spectrum.
In a second embodiment, the change in transmissivity is to electromagnetic radiation
having wavelengths predominately in the visible spectrum. In a third embodiment, the
change in transmissivity is to electromagnetic radiation having wavelengths predominately
in the ultraviolet spectrum. In a fourth embodiment, the change in transmissivity
is to electromagnetic radiation having wavelengths predominately in the ultraviolet
and visible spectra. In a fifth embodiment, the change in transmissivity is to electromagnetic
radiation having wavelengths predominately in the infrared and visible spectra. In
a sixth embodiment, the change in transmissivity is to electromagnetic radiation having
wavelengths predominately in the ultraviolet, visible and infrared spectra.
[0034] The materials making up electrochromic stack 28 may comprise organic or inorganic
materials, and they may be solid or liquid. For example, in certain embodiments the
electrochromic stack 28 comprises materials that are inorganic, solid (
i.e., in the solid state), or both inorganic and solid. Inorganic materials have shown
better reliability in architectural applications. Materials in the solid state can
also offer the advantage of not having containment and leakage issues, as materials
in the liquid state often do. It should be understood that any one or more of the
layers in the stack may contain some amount of organic material, but in many implementations
one or more of the layers contains little or no organic matter. The same can be said
for liquids that may be present in one or more layers in small amounts. In certain
other embodiments some or all of the materials making up electrochromic stack 28 are
organic. Organic ion conductors can offer higher mobilities and thus potentially better
device switching performance. Organic electrochromic layers can provide higher contrast
ratios and more diverse color options. Each of the layers in the electrochromic device
is discussed in detail, below. It should also be understood that solid state material
may be deposited or otherwise formed by processes employing liquid components such
as certain processes employing sol-gels or chemical vapor deposition.
[0035] Referring again to FIG. 1, the power supply (not shown) connected to bus bars 26,
27 is typically a voltage source with optional current limits or current control features
and may be configured to operate in conjunction with local thermal, photosensitive
or other environmental sensors. The voltage source may also be configured to interface
with an energy management system, such as a computer system that controls the electrochromic
device according to factors such as the time of year, time of day, and measured environmental
conditions. Such an energy management system, in conjunction with large area electrochromic
devices (
e.g., an electrochromic architectural window), can dramatically lower the energy consumption
of a building.
[0036] At least one of the substrates 24, 25 is preferably transparent, in order to reveal
the electrochromic properties of the stack 28 to the surroundings. Any material having
suitable optical, electrical, thermal, and mechanical properties may be used as first
substrate 24 or second substrate 25. Such substrates include, for example, glass,
plastic, metal, and metal coated glass or plastic. Non-exclusive examples of possible
plastic substrates are polycarbonates, polyacrylics, polyurethanes, urethane carbonate
copolymers, polysulfones, polyimides, polyacrylates, polyethers, polyester, polyethylenes,
polyalkenes, polyimides, polysulfides, polyvinylacetates and cellulose-based polymers.
If a plastic substrate is used, it may be barrier protected and abrasion protected
using a hard coat of, for example, a diamond-like protection coating, a silica/silicone
anti-abrasion coating, or the like, such as is well known in the plastic glazing art.
Suitable glasses include either clear or tinted soda lime glass, including soda lime
float glass. The glass may be tempered or untempered. In some embodiments of electrochromic
device 1 with glass, e.g. soda lime glass, used as first substrate 24 and/or second
substrate 25, there is a sodium diffusion barrier layer (not shown) between first
substrate 24 and first electrically conductive layer 22 and/or between second substrate
25 and second electrically conductive layer 23 to prevent the diffusion of sodium
ions from the glass into first and/or second electrically conductive layer 23. In
some embodiments, second substrate 25 is omitted.
[0037] In one preferred embodiment of the invention, first substrate 24 and second substrate
25 are each float glass. In certain embodiments for architectural applications, this
glass is at least 0.5 meters by 0.5 meters, and can be much larger,
e.g., as large as about 3 meters by 4 meters. In such applications, this glass is typically
at least about 2 mm thick and more commonly 4-6 mm thick.
[0038] Independent of application, the electrochromic devices of the present invention may
have a wide range of sizes. In general, it is preferred that the electrochromic device
comprise a substrate having a surface with a surface area of at least 0.001 meter
2. For example, in certain embodiments, the electrochromic device comprises a substrate
having a surface with a surface area of at least 0.01 meter
2. By way of further example, in certain embodiments, the electrochromic device comprises
a substrate having a surface with a surface area of at least 0.1 meter
2. By way of further example, in certain embodiments, the electrochromic device comprises
a substrate having a surface with a surface area of at least 1 meter
2. By way of further example, in certain embodiments, the electrochromic device comprises
a substrate having a surface with a surface area of at least 5 meter
2. By way of further example, in certain embodiments, the electrochromic device comprises
a substrate having a surface with a surface area of at least 10 meter
2.
[0039] At least one of the two electrically conductive layers 22, 23 is also preferably
transparent in order to reveal the electrochromic properties of the stack 28 to the
surroundings. In one embodiment, electrically conductive layer 23 is transparent.
In another embodiment, electrically conductive layer 22 is transparent. In another
embodiment, electrically conductive layers 22, 23 are each transparent. In certain
embodiments, one or both of the electrically conductive layers 22, 23 is inorganic
and/or solid. Electrically conductive layers 22 and 23 may be made from a number of
different transparent materials, including transparent conductive oxides, thin metallic
coatings, networks of conductive nano particles (e.g., rods, tubes, dots) conductive
metal nitrides, and composite conductors. Transparent conductive oxides include metal
oxides and metal oxides doped with one or more metals. Examples of such metal oxides
and doped metal oxides include indium oxide, indium tin oxide, doped indium oxide,
tin oxide, doped tin oxide, zinc oxide, aluminum zinc oxide, doped zinc oxide, ruthenium
oxide, doped ruthenium oxide and the like. Transparent conductive oxides are sometimes
referred to as (TCO) layers. Thin metallic coatings that are substantially transparent
may also be used. Examples of metals used for such thin metallic coatings include
gold, platinum, silver, aluminum, nickel, and alloys of these. Examples of transparent
conductive nitrides include titanium nitrides, tantalum nitrides, titanium oxynitrides,
and tantalum oxynitrides. Electrically conducting layers 22 and 23 may also be transparent
composite conductors. Such composite conductors may be fabricated by placing highly
conductive ceramic and metal wires or conductive layer patterns on one of the faces
of the substrate and then over-coating with transparent conductive materials such
as doped tin oxides or indium tin oxide. Ideally, such wires should be thin enough
as to be invisible to the naked eye (
e.g., about 100 µm or thinner). Non-exclusive examples of electron conductors 22 and
23 transparent to visible light are thin films of indium tin oxide (ITO), tin oxide,
zinc oxide, titanium oxide, n- or p-doped zinc oxide and zinc oxyfluoride. Metal-based
layers, such as ZnS/Ag/ZnS and carbon nanotube layers have been recently explored
as well. Depending on the particular application, one or both electrically conductive
layers 22 and 23 may be made of or include a metal grid.
[0040] The thickness of the electrically conductive layer may be influenced by the composition
of the material comprised within the layer and its transparent character. In some
embodiments, electrically conductive layers 22 and 23 are transparent and each have
a thickness that is between about 1000 nm and about 50 nm. In some embodiments, the
thickness of electrically conductive layers 22 and 23 is between about 500 nm and
about 100 nm. In other embodiments, the electrically conductive layers 22 and 23 each
have a thickness that is between about 400 nm and about 200 nm. In general, thicker
or thinner layers may be employed so long as they provide the necessary electrical
properties (
e.g., conductivity) and optical properties (
e.g., transmittance). For certain applications it will generally be preferred that electrically
conductive layers 22 and 23 be as thin as possible to increase transparency and to
reduce cost.
[0041] Referring again to FIG. 1, the function of the electrically conductive layers is
to apply the electric potential provided by a power supply over the entire surface
of the electrochromic stack 28 to interior regions of the stack. The electric potential
is transferred to the conductive layers though electrical connections to the conductive
layers. In some embodiments, bus bars, one in contact with first electrically conductive
layer 22 and one in contact with second electrically conductive layer 23 provide the
electric connection between the voltage source and the electrically conductive layers
22 and 23.
[0042] In one embodiment, the sheet resistance, R
s, of the first and second electrically conductive layers 22 and 23 is about 500 Ω/□
to 1 Ω/□. In some embodiments, the sheet resistance of first and second electrically
conductive layers 22 and 23 is about 100 Ω/□ to 5 Ω/□. In general, it is desirable
that the sheet resistance of each of the first and second electrically conductive
layers 22 and 23 be about the same. In one embodiment, first and second electrically
conductive layers 22 and 23 each have a sheet resistance of about 20 Ω/□ to about
8 Ω/□.
[0043] To facilitate more rapid switching of electrochromic device 1 from a state of relatively
greater transmittance to a state of relatively lesser transmittance, or
vice versa, at least one of electrically conductive layers 22, 23 preferably has a sheet resistance,
R
s, to the flow of electrons through the layer that is non-uniform. For example, in
one embodiment only one of first and second electrically conductive layers 22, 23
has a non-uniform sheet resistance to the flow of electrons through the layer. Alternatively,
and typically more preferably, first electrically conductive layer 22 and second electrically
conductive layer 23 each have a non-uniform sheet resistance to the flow of electrons
through the respective layers. Without being bound by any particular theory, it is
presently believed that spatially varying the sheet resistance of electrically conductive
layer 22, spatially varying the sheet resistance of electrically conductive layer
23, or spatially varying the sheet resistance of electrically conductive layer 22
and electrically conductive layer 23 improves the switching performance of the device
by controlling the voltage drop in the conductive layer to provide uniform potential
drop or a desired non-uniform potential drop across the device, over the area of the
device.
[0044] In general, electrical circuit modeling may be used to determine the sheet resistance
distribution providing desired switching performance, taking into account the type
of electrochromic device, the device shape and dimensions, electrode characteristics,
and the placement of electrical connections (
e.g., bus bars) to the voltage source. The sheet resistance distribution, in turn, can
be controlled, at least in part, by grading the thickness of the first and/or second
electrically conductive layer(s), grading the composition of the first and/or second
electrically conductive layer(s), or patterning the first and/or second electrically
conductive layer(s), or some combination of these.
[0045] In one exemplary embodiment, the electrochromic device is a rectangular electrochromic
window. Referring again to FIG. 1, in this embodiment first substrate 24 and second
substrate 25 are rectangular panes of glass or other transparent substrate and electrochromic
device 1 has two bus bars 26, 27 located on opposite sides of first electrode layer
20 and second electrode layer 21, respectively. When configured in this manner, it
is generally preferred that the resistance to the flow of electrons in first electrically
conductive layer 22 increases with increasing distance from bus bar 26 and that the
resistance to the flow of electrons in second electrically conductive layer 23 increases
with increasing distance from bus bar 27. This, in turn, can be effected, for example,
by decreasing the thickness of first electrically conductive layer 22 as a function
of increasing distance from bus bar 26 and decreasing the thickness of second electrically
conductive layer 23 as a function of increasing distance from bus bar 27.
[0046] The multi-layer devices of the present invention may have a shape other than rectangular,
may have more than two bus bars, and/or may not have the bus bars on opposite sides
of the device. For example, the multi-layer device may have a perimeter that is more
generally a quadrilateral, or a shape with greater or fewer sides than four for example,
the multi-layer device may be triangular, pentagonal, hexagonal,
etc., in shape. By way of further example, the multi-layer device may have a perimeter
that is curved but lacks vertices, e.g., circular, oval, etc. By way of further example,
the multi-layer device may comprise three, four or more bus bars connecting the multi-layer
device to a voltage source, or the bus bars, independent of number may be located
on non-opposing sides. In each of such instances, the preferred resistance profile
in the electrically conductive layer(s) may vary from that which is described for
the rectangular, two bus bar configuration.
[0047] In general, however, and independent of whether the multi-layer device has a shape
other than rectangular, there are more than two electrical connections (
e.g., bus bars), and/or the electrical connections (
e.g., bus bars) are on opposite sides of the device, the sheet resistance, R
s, in the first electrically conductive layer 22, in the second electrically conductive
layer 23, or in the first electrically conductive layer 22 and the second electrically
conductive layer 23 may be plotted to join points of equal sheet resistance (
i.e., isoresistance lines) as a function of (two-dimensional) position within the first
and/or second electrically conductive layer. Plots of this general nature, sometimes
referred to as contour maps, are routinely used in cartography to join points of equal
elevation. In the context of the present invention, a contour map of the sheet resistance,
R
s, in the first and/or second electrically conductive layer as a function of (two-dimensional)
position within the first and/or second electrically conductive layer preferably contains
a series of isoresistance lines (also sometimes referred to as contour lines) and
resistance gradient lines (lines perpendicular to the isoresistance lines). The sheet
resistance along a gradient line in the first and/or second electrically conductive
layer(s) generally increase(s), generally decrease(s), generally increase(s) until
it reaches a maximum and then generally decrease(s), or generally decrease(s) until
it reaches a minimum and then generally increase(s).
[0048] Figs. 2A - 2E depict a contour map of the sheet resistance, R
s, in an electrically conductive layer (
i.e., the first electrically conductive layer, the second electrically conductive layer,
or each of the first and second electrically conductive layers) as a function of (two-dimensional)
position within the electrically conductive layer for several exemplary embodiments
of an electrochromic stack in accordance with the present invention. In each of Figs.
2A - 2E, contour map 50 depicts a set of sheet isoresistance curves 52 (
i.e., curves along which the sheet resistance, R
s, has a constant value) and a set of resistance gradient curves 54 that are perpendicular
to isoresistance curves 52 resulting from an electrochromic stack having a perimeter
that is square (Figs. 2A, 2B, and 2C) or circular (Figs. 2D and 2E) and varying numbers
and locations of bus bars 226 and 227 in contact with the first and second electrically
conductive layers (not labeled) of the electrochromic stack. In FIG. 2A, the direction
of the set of gradients 54 indicates that the sheet resistance, R
s, within the electrically conductive layer progressively increases along the set of
gradients 54 and between west side 55 and east side 56 of the electrically conductive
layer in contact with bus bar 227. In FIG. 2B, the direction of gradient 54A indicates
that the sheet resistance, R
s, within the electrically conductive layer in contact with bus bar 227 progressively
decreases from southwest corner 57 to centroid 59 and then decreases from centroid
59 to northeast corner 58. In FIG. 2C, the direction of the set of gradients 54 indicate
that the sheet resistance, R
s, within the electrically conductive layer in contact with bus bar 227 progressively
decreases from the west side 60 and east side 61 to centroid 59 and progressively
increases from the top side 58 and bottom side 57 to centroid 59; stated differently,
sheet resistance, R
s, forms a saddle like form centered around centroid 59. In FIG. 2D, the direction
of gradients 54a and 54b indicates that the sheet resistance, R
s, within the electrically conductive layer in contact with bus bar 227 progressively
decreases from each of positions 64 and 65 to centroid 59 and progressively increases
from each of positions 63 and 62 to centroid 59; stated differently, sheet resistance,
R
s, forms a saddle like form centered around centroid 59. In FIG. 2E, the direction
of the set of gradients 54 indicates that the sheet resistance, R
s, within the electrically conductive layer in contact with bus bar 227 progressively
decreases from the west side 55 to the east side 56. In one embodiment, for example,
the gradient in sheet resistance is a constant. By way of further example, in one
embodiment, the gradient in sheet resistance is a constant and the substrate is rectangular
in shape
[0049] In one presently preferred embodiment, the ratio of the value of maximum sheet resistance,
R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 1.25. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 1.5. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 2. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 3. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 4. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 5. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 6. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 7. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 8. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 9. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer is at least about 10.
[0050] FIG. 21 illustrates the non-uniformity in the sheet resistance of first electrically
conductive layer 22 of multi-layer electrochromic device 1. First electrically conductive
layer 22 comprises a sheet resistance gradient curve (the line comprising line segment
X
1-Y
1, indicating that the sheet resistance, R
s, within electrically conductive layer 22 progressively increases as described in
connection with FIG. 2). Between X
1 and Y
1, the sheet resistance of first electrically conductive layer 22 generally increases,
generally decreases or generally increases and then decreases. In one embodiment,
line segment X
1-Y
1 has a length of at least 1 cm. For example, line segment X
1-Y
1 may have a length of 2.5 cm, 5 cm, 10 cm, or 25 cm. Additionally, line segment X
1-Y
1 may be straight or curved.
[0051] In one embodiment, the non-uniformity in the sheet resistance of the first electrically
conductive layer may be observed by comparing the ratio of the average sheet resistance,
R
avg in two different regions of the first electrically conductive layer wherein the first
and second regions are each circumscribed by a convex polygon and each comprises at
least 25% of the surface area of the first electrically conductive layer. For example,
in one such embodiment, the ratio of the average sheet resistance in a first region
of the first electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 1.25 wherein each of the first and second regions is circumscribed by
a convex polygon, and each comprises at least 25% of the surface area of the first
electrically conductive layer. This may be illustrated by reference to FIG. 21. First
electrically conductive layer 22 comprises convex polygon A
1 and convex polygon B
1 and each circumscribes a region comprising at least 25% of the surface area of first
electrically conductive layer 22; in one embodiment, the ratio of the average sheet
resistance, R
1avg, in a first region of the first electrically conductive layer bounded by convex polygon
A
1 to the average sheet resistance, R
2avg, in a second region of the first electrically conductive layer bounded by convex
polygon B
1 is at least 1.25. As illustrated, convex polygon A
1 is a triangle and convex polygon B
1 is a square merely for purposes of exemplification; in practice, the first region
may be bounded by any convex polygon and the second region may be bounded by any convex
polygon. By way of further example, in one such embodiment, the ratio of the average
sheet resistance in a first region of the first electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 1.5 wherein the first and second regions are each circumscribed by a
convex polygon and each comprises at least 25% of the surface area of the first electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 2 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the first electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 3 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the first electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 4 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the first electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 5 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the first electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 6 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the first electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 7 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the first electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 8 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the first electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 9 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the first electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 10 wherein the first and second regions are each circumscribed by a
convex polygon and each comprises at least 25% of the surface area of the first electrically
conductive layer. In one embodiment in each of the foregoing examples, the first and
second regions are mutually exclusive regions.
[0052] In one embodiment, the non-uniformity in the sheet resistance of the first electrically
conductive layer may be observed by comparing the average sheet resistance, R
avg in four different regions of the first electrically conductive layer wherein the
first region is contiguous with the second region, the second region is contiguous
with the third region, the third region is contiguous with the fourth region, each
of the regions is circumscribed by a convex polygon, and each comprises at least 10%
of the surface area of the first electrically conductive layer. For example, in one
such embodiment, the ratio of the average sheet resistance in a first region of the
first electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 1.25, the ratio of the average sheet resistance in the second region
of the first electrically conductive layer, R
2avg, to the average sheet resistance in a third region of the first electrically conductive
layer, R
3avg, is at least 1.25, the ratio of the average sheet resistance in the third region
of the first electrically conductive layer, R
3avg, to the average sheet resistance in a fourth region of the first electrically conductive
layer, R
4avg, is at least 1.25, wherein the first region is contiguous with the second region,
the second region is contiguous with the third region, the third region is contiguous
with the fourth region, each of the regions is circumscribed by a convex polygon,
and each comprises at least 10% of the surface area of the first electrically conductive
layer. By way of further example, in one such embodiment, the ratio of the average
sheet resistance in a first region of the first electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 1.5, the ratio of the average sheet resistance in the second region
of the first electrically conductive layer, R
2avg, to the average sheet resistance in a third region of the first electrically conductive
layer, R
3avg, is at least 1.5, the ratio of the average sheet resistance in the third region of
the first electrically conductive layer, R
3avg, to the average sheet resistance in a fourth region of the first electrically conductive
layer, R
4avg, is at least 1.5, wherein the first region is contiguous with the second region,
the second region is contiguous with the third region, the third region is contiguous
with the fourth region, each of the regions is circumscribed by a convex polygon,
and each comprises at least 10% of the surface area of the first electrically conductive
layer. By way of further example, in one such embodiment, the ratio of the average
sheet resistance in a first region of the first electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 2, the ratio of the average sheet resistance in the second region of
the first electrically conductive layer, R
2avg, to the average sheet resistance in a third region of the first electrically conductive
layer, R
3avg, is at least 2, the ratio of the average sheet resistance in the third region of
the first electrically conductive layer, R
3avg, to the average sheet resistance in a fourth region of the first electrically conductive
layer, R
4avg, is at least 2, wherein the first region is contiguous with the second region, the
second region is contiguous with the third region, the third region is contiguous
with the fourth region, each of the regions is circumscribed by a convex polygon,
and each comprises at least 10% of the surface area of the first electrically conductive
layer. In one embodiment in each of the foregoing examples, the first, second, third
and fourth regions are mutually exclusive regions.
[0053] In one presently preferred embodiment, the second electrically conductive layer has
a sheet resistance, R
s, to the flow of electrical current through the second electrically conductive layer
that varies as a function of position in the second electrically conductive layer.
In one such embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer is at least about 1.25. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer is at least about 1.5. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer is at least about 2. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer is at least about 3. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer is at least about 4. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer is at least about 5. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer is at least about 6. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer is at least about 7. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer is at least about 8. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer is at least about 9. In one exemplary
embodiment, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer is at least about 10.
[0054] FIG. 21 illustrates the non-uniformity in the sheet resistance of second electrically
conductive layer 23 of multi-layer electrochromic device 1. Electrically conductive
layer 22 comprises sheet resistance gradient curve 54 which includes line segment
X-Y; between X and Y, the sheet resistance of second electrically conductive layer
23 generally increases, generally decreases or generally increases and then decreases.
In one embodiment, line segment X
1-Y
1 has a length of at least 1 cm. For example, line segment X-Y may have a length of
2.5 cm, 5 cm, 10 cm, or 25 cm. Additionally, line segment X-Y may be straight or curved.
[0055] In one embodiment, the non-uniformity in the sheet resistance of the second electrically
conductive layer may be observed by comparing the ratio of the average sheet resistance,
R
avg in two different regions of the second electrically conductive layer wherein the
first and second regions are each circumscribed by a convex polygon and each comprises
at least 25% of the surface area of the second electrically conductive layer. For
example, in one such embodiment, the ratio of the average sheet resistance in a first
region of the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 1.25 wherein the first and second regions are each circumscribed by
a convex polygon and each comprises at least 25% of the surface area of the second
electrically conductive layer. This may be illustrated by reference to FIG. 21. Second
electrically conductive layer 23 comprises convex polygon A and convex polygon B and
each circumscribes a region comprising at least 25% of the surface area of second
electrically conductive layer 23; in one embodiment, the ratio of the average sheet
resistance, R
1avg, in a first region of the second electrically conductive layer bounded by convex
polygon A to the average sheet resistance, R
2avg, in a second region of the second electrically conductive layer bounded by convex
polygon B is at least 1.25. As illustrated, convex polygon A is a triangle and convex
polygon B is a square merely for purposes of exemplification; in practice, the first
region may be bounded by any convex polygon and the second region may be bounded by
any convex polygon. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the second electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 1.5 wherein the first and second regions are each circumscribed by a
convex polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the second electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 2 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the second electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 3 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the second electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 4 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the second electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 5 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the second electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 6 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the second electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 7 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the second electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 8 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the second electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 9 wherein the first and second regions are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the second electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 10 wherein the first and second regions are each circumscribed by a
convex polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. In one embodiment in each of the foregoing examples, the first and
second regions are mutually exclusive regions.
[0056] In one embodiment, the non-uniformity in the sheet resistance of the second electrically
conductive layer may be observed by comparing the average sheet resistance, R
avg in four different regions of the second electrically conductive layer wherein the
first region is contiguous with the second region, the second region is contiguous
with the third region, the third region is contiguous with the fourth region, each
of the regions is circumscribed by a convex polygon, and each comprises at least 10%
of the surface area of the second electrically conductive layer. For example, in one
such embodiment, the ratio of the average sheet resistance in a first region of the
second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 1.25, the ratio of the average sheet resistance in the second region
of the second electrically conductive layer, R
2avg, to the average sheet resistance in a third region of the second electrically conductive
layer, R
3avg, is at least 1.25, the ratio of the average sheet resistance in the third region
of the second electrically conductive layer, R
3avg, to the average sheet resistance in a fourth region of the second electrically conductive
layer, R
4avg, is at least 1.25, wherein the first region is contiguous with the second region,
the second region is contiguous with the third region, the third region is contiguous
with the fourth region, each of the regions is circumscribed by a convex polygon,
and each comprises at least 10% of the surface area of the second electrically conductive
layer. By way of further example, in one such embodiment, the ratio of the average
sheet resistance in a first region of the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 1.5, the ratio of the average sheet resistance in the second region
of the second electrically conductive layer, R
2avg, to the average sheet resistance in a third region of the second electrically conductive
layer, R
3avg, is at least 1.5, the ratio of the average sheet resistance in the third region of
the second electrically conductive layer, R
3avg, to the average sheet resistance in a fourth region of the second electrically conductive
layer, R
4avg, is at least 1.5, wherein the first region is contiguous with the second region,
the second region is contiguous with the third region, the third region is contiguous
with the fourth region, each of the regions is circumscribed by a convex polygon,
and each comprises at least 10% of the surface area of the second electrically conductive
layer. By way of further example, in one such embodiment, the ratio of the average
sheet resistance in a first region of the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 2, the ratio of the average sheet resistance in the second region of
the second electrically conductive layer, R
2avg, to the average sheet resistance in a third region of the second electrically conductive
layer, R
3avg, is at least 2, the ratio of the average sheet resistance in the third region of
the second electrically conductive layer, R
3avg, to the average sheet resistance in a fourth region of the second electrically conductive
layer, R
4avg, is at least 2, wherein the first region is contiguous with the second region, the
second region is contiguous with the third region, the third region is contiguous
with the fourth region, each of the regions is circumscribed by a convex polygon,
and each comprises at least 10% of the surface area of the second electrically conductive
layer. In one embodiment in each of the foregoing examples, the first, second, third
and fourth regions are mutually exclusive regions.
[0057] In one presently preferred embodiment, first and second electrically conductive layers
22, 23 have a sheet resistance, R
s, to the flow of electrical current through the second electrically conductive layer
that varies as a function of position in the first and second electrically conductive
layers. Although it is generally preferred in this embodiment that the ratio of the
value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first and second electrically conductive layers be approximately the same,
they may have different values. For example, in one such embodiment, the ratio of
the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first electrically conductive layer has a value that is at least twice as
much as the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the second electrically conductive layer. More typically, however, the ratio
of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first and second electrically conductive layers will be approximately the
same and each at least about 1.25. In one exemplary embodiment, the ratio of the value
of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in the first and second electrically conductive layers will be approximately the
same and each at least about 1.5. In one exemplary embodiment, the ratio of the value
of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in each of the first and second electrically conductive layers is at least about
2. In one exemplary embodiment, the ratio of the value of maximum sheet resistance,
R
max, to the value of minimum sheet resistance, R
min, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in each of the first and second electrically conductive layers is at least about
3. In one exemplary embodiment, the ratio of the value of maximum sheet resistance,
R
max, to the value of minimum sheet resistance, R
min, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in each of the first and second electrically conductive layers is at least about
4. In one exemplary embodiment, the ratio of the value of maximum sheet resistance,
R
max, to the value of minimum sheet resistance, R
min, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in each of the first and second electrically conductive layers is at least about
5. In one exemplary embodiment, the ratio of the value of maximum sheet resistance,
R
max, to the value of minimum sheet resistance, R
min, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in each of the first and second electrically conductive layers is at least about
6. In one exemplary embodiment, the ratio of the value of maximum sheet resistance,
R
max, to the value of minimum sheet resistance, R
min, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in each of the first and second electrically conductive layers is at least about
7. In one exemplary embodiment, the ratio of the value of maximum sheet resistance,
R
max, to the value of minimum sheet resistance, R
min, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in each of the first and second electrically conductive layers is at least about
8. In one exemplary embodiment, the ratio of the value of maximum sheet resistance,
R
max, to the value of minimum sheet resistance, R
min, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in each of the first and second electrically conductive layers is at least about
9. In one exemplary embodiment, the ratio of the value of maximum sheet resistance,
R
max, to the value of minimum sheet resistance, R
min, the ratio of the value of maximum sheet resistance, R
max, to the value of minimum sheet resistance, R
min, in each of the first and second electrically conductive layers is at least about
10.
[0058] In one embodiment, the non-uniformity in the sheet resistance of the first and second
electrically conductive layers may be observed by comparing the ratio of the average
sheet resistance, R
avg in two different regions of the first and second electrically conductive layers,
respectively, wherein the first and second regions of the first electrically conductive
layer are each circumscribed by a convex polygon and each comprises at least 25% of
the surface area of the first electrically conductive layer and the first and second
regions of the second electrically conductive layer are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. For example, in one such embodiment, the ratio of the average sheet
resistance in a first region of the first electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 1.25 and the ratio of the average sheet resistance in a first region
of the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 1.25 wherein the first and second regions of the first electrically
conductive layer are each circumscribed by a convex polygon and each comprises at
least 25% of the surface area of the first electrically conductive layer and the first
and second regions of the second electrically conductive layer are each circumscribed
by a convex polygon and each comprises at least 25% of the surface area of the second
electrically conductive layer. By way of further example, in one such embodiment,
the ratio of the average sheet resistance in a first region of the first electrically
conductive layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 1.5 and the ratio of the average sheet resistance in a first region
of the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 1.5 wherein the first and second regions of the first electrically conductive
layer are each circumscribed by a convex polygon and each comprises at least 25% of
the surface area of the first electrically conductive layer and the first and second
regions of the second electrically conductive layer are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 2 and the ratio of the average sheet resistance in a first region of
the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 2 wherein the first and second regions of the first electrically conductive
layer are each circumscribed by a convex polygon and each comprises at least 25% of
the surface area of the first electrically conductive layer and the first and second
regions of the second electrically conductive layer are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 3 and the ratio of the average sheet resistance in a first region of
the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 3 wherein the first and second regions of the first electrically conductive
layer are each circumscribed by a convex polygon and each comprises at least 25% of
the surface area of the first electrically conductive layer and the first and second
regions of the second electrically conductive layer are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 4 and the ratio of the average sheet resistance in a first region of
the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 4 wherein the first and second regions of the first electrically conductive
layer are each circumscribed by a convex polygon and each comprises at least 25% of
the surface area of the first electrically conductive layer and the first and second
regions of the second electrically conductive layer are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 5 and the ratio of the average sheet resistance in a first region of
the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 5 wherein the first and second regions of the first electrically conductive
layer are each circumscribed by a convex polygon and each comprises at least 25% of
the surface area of the first electrically conductive layer and the first and second
regions of the second electrically conductive layer are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 6 and the ratio of the average sheet resistance in a first region of
the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 6 wherein the first and second regions of the first electrically conductive
layer are each circumscribed by a convex polygon and each comprises at least 25% of
the surface area of the first electrically conductive layer and the first and second
regions of the second electrically conductive layer are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 7 and the ratio of the average sheet resistance in a first region of
the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 7 wherein the first and second regions of the first electrically conductive
layer are each circumscribed by a convex polygon and each comprises at least 25% of
the surface area of the first electrically conductive layer and the first and second
regions of the second electrically conductive layer are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 8 and the ratio of the average sheet resistance in a first region of
the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 8 wherein the first and second regions of the first electrically conductive
layer are each circumscribed by a convex polygon and each comprises at least 25% of
the surface area of the first electrically conductive layer and the first and second
regions of the second electrically conductive layer are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 9 and the ratio of the average sheet resistance in a first region of
the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 9 wherein the first and second regions of the first electrically conductive
layer are each circumscribed by a convex polygon and each comprises at least 25% of
the surface area of the first electrically conductive layer and the first and second
regions of the second electrically conductive layer are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. By way of further example, in one such embodiment, the ratio of
the average sheet resistance in a first region of the first electrically conductive
layer, R
1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R
2avg, is at least 10 and the ratio of the average sheet resistance in a first region of
the second electrically conductive layer, R
1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R
2avg, is at least 10 wherein the first and second regions of the first electrically conductive
layer are each circumscribed by a convex polygon and each comprises at least 25% of
the surface area of the first electrically conductive layer and the first and second
regions of the second electrically conductive layer are each circumscribed by a convex
polygon and each comprises at least 25% of the surface area of the second electrically
conductive layer. In one embodiment in each of the foregoing examples, the first and
second regions are mutually exclusive regions.
[0059] Referring again to FIG. 21, the spatial non-uniformity of the sheet resistance of
the first and second electrically conductive layer may be correlated in accordance
with one aspect of the present invention. For example, line segment X
1-Y
1 in first electrically conductive layer 22 may be projected through second electrode
layer 21, ion conductor layer 10 and first electrode layer 20 and onto second electrically
conductive layer 23, with the projection defining line segment X-Y. In general, if
the sheet resistance generally increases in first electrically conductive layer 22
along line segment X
1-Y
1 (
i.e., the sheet resistance generally increases moving along the sheet resistance gradient
curve in the direction from point X
1 to point Y
1), the sheet resistance generally decreases in second electrically conductive layer
23 along segment X-Y (
i.e., the sheet resistance generally decreases along sheet resistance gradient curve
54 and in the direction from point X to point Y). As previously noted, line segments
X-Y and X
1-Y
1 have a length of at least 1 cm. For example, line segments X-Y and X
1-Y
1 may have a length of 2.5 cm, 5 cm, 10 cm, or 25 cm. Additionally, line segments X-Y
and X
1-Y
1 may be straight or curved. In one embodiment, for example, the sheet resistance gradients
in electrically conductive layers 22, 23 are non-zero constants and are of opposite
sign (
e.g., the sheet resistance generally increases linearly in first electrically conductive
layer along in the direction from point X
1 to point Y
1 and generally decreases linearly along sheet resistance gradient curve 54 in the
direction from point X to point Y). By way of further example, in one embodiment,
substrates 24, 25 are rectangular and the sheet resistance gradients in electrically
conductive layers 22, 23 are non-zero constants and are of opposite sign (
e.g., the sheet resistance generally increases linearly in second electrically conductive
layer 23 along gradient 54 in the direction from point X to point Y and generally
decreases linearly in first electrically conductive layer 22 along the line containing
line segment X
1-Y
1 in the direction from point X
1 to point Y
1).
[0060] In another embodiment, and still referring to FIG. 21, the spatial non-uniformity
of the sheet resistance of the first and second electrically conductive layers may
be characterized by reference to separate first and second regions in the first electrically
conductive layer and their projections onto the second electrically conductive layer
to define complementary first and second regions in the second electrically conductive
layer wherein the first and second regions of the first electrically conductive layer
are each bounded by a convex polygon, each contain at least 25% of the surface area
of the first electrically conductive layer, and are mutually exclusive regions. In
general, the first electrically conductive layer has an average sheet resistance in
the first and regions of the first electrically conductive layer and the second electrically
conductive layer has an average sheet resistance in the complementary first and second
regions of the second electrically conductive layer wherein: (a) (i) a ratio of the
average sheet resistance of the first electrically conductive layer in the first region
to the average sheet resistance of the first electrically conductive layer in the
second region is at least 1.5 or (ii) a ratio of the average sheet resistance of the
second electrically conductive layer in the complementary first region to the average
sheet resistance of the second electrically conductive layer in the complementary
second region is greater than 1.5 and (b) a ratio of the average sheet resistance
of the first electrically conductive layer in the first region to the average sheet
resistance of the second electrically layer in the complementary first region (
i.e., the projection of the first region of the first electrically conductive layer onto
the second electrically conductive layer) is at least 150% of the ratio of the average
sheet resistance of the first electrically conductive layer in the second region to
the average sheet resistance of the second electrically layer in the complementary
second region (
i.e., the projection of the second region of the first electrically conductive layer
onto the second electrically conductive layer).
[0061] Referring again to FIG. 21, first electrically conductive layer 22 comprises a region
A
1 and a region B
1 wherein region A
1 and region B
1 each comprise at least 25% of the surface area of the first electrically conductive
layer, are each circumscribed by a convex polygon and are mutually exclusive regions.
A projection of region A
1 onto second electrically conductive layer 23 defines a region A circumscribed by
a convex polygon in the second electrically conductive layer comprising at least 25%
of the surface area of the second electrically conductive layer. A projection of region
B
1 onto the second electrically conductive layer defines a region B circumscribed by
a convex polygon in the second electrically conductive layer comprising at least 25%
of the surface area of the second electrically conductive layer. First electrically
conductive layer 22 has an average sheet resistance in region A
1 corresponding to R
A1avg and an average sheet resistance in region B
1 corresponding to R
B1avg. Second electrically conductive layer 23 has an average sheet resistance in region
A corresponding to R
Aavg and an average sheet resistance in region B corresponding to R
Bavg. In accordance with one embodiment, (i) the ratio of R
A1avg to R
B1avg or the ratio of R
Bavg to R
Aavg is at least 1.5 and (ii) the ratio of (R
A1avg/R
Aavg) to (R
B1avg/R
Bavg) is at least 1.5. For example, in one embodiment, (i) the ratio of R
A1avg to R
B1avg or the ratio of R
Bavg to R
Aavg is at least 1.75 and (ii) the ratio of (R
A1avg/R
Aavg) to (R
B1avg/R
Bavg) is at least 1.75. By way of further example, in one embodiment, (i) the ratio of
R
A1avg to R
B1avg or the ratio of R
Bavg to R
Aavg is at least 2 and (ii) the ratio of (R
A1avg/R
Aavg) to (R
B1avg/R
Bavg) is at least 2. By way of further example, in one embodiment, (i) the ratio of R
A1avg to R
B1avg or the ratio of R
Bavg to R
Aavg is at least 3 and (ii) the ratio of (R
A1avg/R
Aavg) to (R
B1avg/R
Bavg) is at least 3. By way of further example, in one embodiment, (i) the ratio of R
A1avg to R
B1avg or the ratio of R
Bavg to R
Aavg is at least 5 and (ii) the ratio of (R
A1avg/R
Aavg) to (R
B1avg/R
Bavg) is at least 5. By way of further example, in one embodiment, (i) the ratio of R
A1avg to R
B1avg or the ratio of R
Bavg to R
Aavg is at least 10 and (ii) the ratio of (R
A1avg/R
Aavg) to (R
B1avg/R
Bavg) is at least 10.
[0062] Without wishing to be bound by any particular theory, and based upon certain experimental
evidence obtained to-date, in certain embodiments the electrode sheet resistance may
be expressed as a function of position in a large area electrochromic device that
provides a local voltage drop across the electrochromic stack that is substantially
constant. For the simple geometry shown in Figure 1, where the contact (bus bar 27)
to the top electrode is made at x = 0 and the contact (bus bar 26) to the bottom electrode
is made at x = xt, the relationship is simply that

where R(x) is the sheet resistance of the top electrode as a function of position
and R'(x) is the sheet resistance of the bottom electrode as a function of position.
A simple mathematical example of this relationship is that for a linear change in
the sheet resistance of the top electrode, R(x) = a*x, the sheet resistance of the
bottom electrode must be R'(x) = a*(xt-x). Another simple example is that for R(x)
= 1/(xt-a*x) then R'(x) = 1/(a*x). This relationship holds in a mathematical sense
for any function R(x). This relationship can be generalized to any electrode sheet
resistance distribution that smoothly varies and any contact configuration by the
following relationship between the sheet resistance from one contact (z=0) to anther
(z=L) along gradient curves that are perpendicular to iso-resistance lines R(z), and
the corresponding opposing electrode sheet resistance distribution R'(z).

As a practical matter, devices do not need to precisely adhere to this relationship
to realize the benefits of this invention. For example, in the case above where R'(x)
= 1/(a*x), R'(0) = infinity. While one can practically create resistances of very
large magnitude, a film with a R'(x) = 1/(a*x+b) where b is small relative to a can
exhibit significantly improved switching uniformity over a device comprising electrodes
of uniform sheet resistance.
[0063] Electrically conductive layers having a non-uniform sheet resistance may be prepared
by a range of methods. In one embodiment, the non-uniform sheet resistance is the
result of a composition variation in the layer; composition variations may be formed,
for example, by sputter coating from two cylindrical targets of different materials
while varying the power to each target as a function of position relative to the substrate,
by reactive sputter coating from a cylindrical target while varying the gas partial
pressure and/or composition as a function of position relative to the substrate, by
spray coating with a varying composition or process as a function of position relative
to the substrate, or by introducing a dopant variation to a uniform composition and
thickness film by ion implantation, diffusion, or reaction. In another embodiment,
the non-uniform sheet resistance is the result of a thickness variation in the layer;
thickness variations may be formed, for example, by sputter coating from a cylindrical
target while varying the power to the target as a function of as a function of position
relative to the substrate, sputter coating from a target at constant power and varying
the velocity of substrate under the target as a function of as a function of position
relative to the substrate, a deposited stack of uniform TCO films 222a - 222r on substrate
224 where each film has a limited spatial extent as illustrated in FIG. 3. Alternatively,
a thickness gradient can be formed by starting with a uniform thickness conductive
layer and then etching the layer in a way that is spatially non-uniform such as dip-etching
or spraying with etchant at a non-uniform rate across the layer. In another embodiment,
the non-uniform sheet resistance is the result of patterning; gradients may be introduced,
for example, by laser patterning a series of scribes into a constant thickness and
constant resistivity film to create a desired spatially varying resistivity. In addition
to laser patterning, mechanical scribing and lithographic patterning using photoresists
(as known in the art of semiconductor device manufacturing) can be used to create
a desired spatially varying resistivity. In another embodiment, the non-uniform sheet
resistance is the result of a defect variation; a defect variation may be introduced,
for example, by introducing spatially varying defects via ion implantation, or creating
a spatially varying defect density via a spatially varying annealing process applied
to a layer with a previously uniform defect density.
[0064] Referring again to FIG. 1, at least one of first and second electrode layers 20 and
21 is electrochromic, one of the first and second electrode layers is the counter
electrode for the other, and first and second electrode layers 20 and 21 are inorganic
and/or solid. Non-exclusive examples of electrochromic electrode layers 20 and 21
are cathodically coloring thin films of oxides based on tungsten, molybdenum, niobium,
titanium, lead and/or bismuth, or anodically coloring thin films of oxides, hydroxides
and/or oxy-hydrides based on nickel, iridium, iron, chromium, cobalt and/or rhodium.
[0065] In one embodiment, first electrode layer 20 contains any one or more of a number
of different electrochromic materials, including metal oxides. Such metal oxides include
tungsten oxide (WO
3), molybdenum oxide (MoO
3), niobium oxide (Nb
2O
5), titanium oxide (TiO
2), copper oxide (CuO), iridium oxide (Ir
2O
3), chromium oxide (Cr
2O
3), manganese oxide (Mn
2O
3), vanadium oxide (V
2O
3), nickel oxide (Ni
2O
3), cobalt oxide (Co
2O
3) and the like. In some embodiments, the metal oxide is doped with one or more dopants
such as lithium, sodium, potassium, molybdenum, vanadium, titanium, and/or other suitable
metals or compounds containing metals. Mixed oxides (
e.g., W--Mo oxide, W-V oxide) are also used in certain embodiments.
[0066] In some embodiments, tungsten oxide or doped tungsten oxide is used for first electrode
layer 20. In one embodiment, first electrode layer 20 is electrochromic and is made
substantially of WO
x, where "x" refers to an atomic ratio of oxygen to tungsten in the electrochromic
layer, and x is between about 2.7 and 3.5. It has been suggested that only sub-stoichiometric
tungsten oxide exhibits electrochromism;
i.e., stoichiometric tungsten oxide, WO
3, does not exhibit electrochromism. In a more specific embodiment, WO
x, where x is less than 3.0 and at least about 2.7 is used for first electrode layer
20. In another embodiment, first electrode layer 20 is WO
x, where x is between about 2.7 and about 2.9. Techniques such as Rutherford Backscattering
Spectroscopy (RBS) can identify the total number of oxygen atoms which include those
bonded to tungsten and those not bonded to tungsten. In some instances, tungsten oxide
layers where x is 3 or greater exhibit electrochromism, presumably due to unbound
excess oxygen along with sub-stoichiometric tungsten oxide. In another embodiment,
the tungsten oxide layer has stoichiometric or greater oxygen, where x is 3.0 to about
3.5.
[0067] In certain embodiments, the electrochromic mixed metal oxide is crystalline, nanocrystalline,
or amorphous. In some embodiments, the tungsten oxide is substantially nanocrystalline,
with grain sizes, on average, from about 5 nm to 50 nm (or from about 5 nm to 20 nm),
as characterized by transmission electron microscopy (TEM). The tungsten oxide morphology
may also be characterized as nanocrystalline using x-ray diffraction (XRD); XRD. For
example, nanocrystalline electrochromic tungsten oxide may be characterized by the
following XRD features: a crystal size of about 10 to 100 nm (
e.g., about 55 nm. Further, nanocrystalline tungsten oxide may exhibit limited long range
order,
e.g., on the order of several (about 5 to 20) tungsten oxide unit cells.
[0068] The thickness of the first electrode layer 20 depends on the electrochromic material
selected for the electrochromic layer. In some embodiments, first electrode layer
20 is about 50 nm to 2,000 nm, or about 100 nm to 700 nm. In some embodiments, the
first electrode layer 20 is about 250 nm to about 500 nm.
[0069] Second electrode layer 21 serves as the counter electrode to first electrode layer
20 and, like first electrode layer 20, second electrode layer 21 may comprise electrochromic
materials as well as non-electrochromic materials. Non-exclusive examples of second
electrode layer 21 are cathodically coloring electrochromic thin films of oxides based
on tungsten, molybdenum, niobium, titanium, lead and/or bismuth, anodically coloring
electrochromic thin films of oxides, hydroxides and/or oxy-hydrides based on nickel,
iridium, iron, chromium, cobalt and/or rhodium, or non-electrochromic thin films,
e.g., of oxides based on vanadium and/or cerium as well as activated carbon. Also combinations
of such materials can be used as second electrode layer 21.
[0070] In some embodiments, second electrode layer 21 may comprise one or more of a number
of different materials that are capable of serving as reservoirs of ions when the
electrochromic device is in the bleached state. During an electrochromic transition
initiated by,
e.g., application of an appropriate electric potential, the counter electrode layer transfers
some or all of the ions it holds to the electrochromic first electrode layer 20, changing
the electrochromic first electrode layer 20 to the colored state.
[0071] In some embodiments, suitable materials for a counter electrode complementary to
WO
3 include nickel oxide (NiO), nickel tungsten oxide (NiWO), nickel vanadium oxide,
nickel chromium oxide, nickel aluminum oxide, nickel manganese oxide, nickel magnesium
oxide, chromium oxide (Cr
2O
3), manganese oxide (MnO
2), and Prussian blue. Optically passive counter electrodes comprise cerium titanium
oxide (CeO
2--TiO
2), cerium zirconium oxide (CeO
2--ZrO
2), nickel oxide (NiO), nickel-tungsten oxide (NiWO), vanadium oxide (V
2O
5), and mixtures of oxides (
e.g., a mixture of Ni
2O
3 and WO
3). Doped formulations of these oxides may also be used, with dopants including,
e.g., tantalum and tungsten. Because first electrode layer 20 contains the ions used
to produce the electrochromic phenomenon in the electrochromic material when the electrochromic
material is in the bleached state, the counter electrode preferably has high transmittance
and a neutral color when it holds significant quantities of these ions.
[0072] In some embodiments, nickel-tungsten oxide (NiWO) is used in the counter electrode
layer. In certain embodiments, the amount of nickel present in the nickel-tungsten
oxide can be up to about 90% by weight of the nickel-tungsten oxide. In a specific
embodiment, the mass ratio of nickel to tungsten in the nickel-tungsten oxide is between
about 4:6 and 6:4 (e.g., about 1:1). In one embodiment, the NiWO is between about
15% (atomic) Ni and about 60% Ni; between about 10% W and about 40% W; and between
about 30% O and about 75% O. In another embodiment, the NiWO is between about 30%
(atomic) Ni and about 45% Ni; between about 10% W and about 25% W; and between about
35% O and about 50% O. In one embodiment, the NiWO is about 42% (atomic) Ni, about
14% W, and about 44% O.
[0073] In some embodiments, the thickness of second electrode layer 21 is about 50 nm about
650 nm. In some embodiments, the thickness of second electrode layer 21 is about 100
nm to about 400 nm, preferably in the range of about 200 nm to 300 nm.
[0074] Ion conducting layer 10 serves as a medium through which ions are transported (in
the manner of an electrolyte) when the electrochromic device transforms between the
bleached state and the colored state. Ion conductor layer 10 comprises an ion conductor
material. It may be transparent or non-transparent, colored or non-colored, depending
on the application. Preferably, ion conducting layer 10 is highly conductive to the
relevant ions for the first and second electrode layers 20 and 21. Depending on the
choice of materials, such ions include lithium ions (Li
+) and hydrogen ions (H
+) (
i.e., protons). Other ions may also be employed in certain embodiments. These include
deuterium ions (D
+), sodium ions (Na
+), potassium ions (K
+), calcium ions (Ca
++), barium ions (Ba
++), strontium ions (Sr
++), and magnesium ions (Mg
++). Preferably, ion conducting layer 10 also has sufficiently low electron conductivity
that negligible electron transfer takes place during normal operation. In various
embodiments, the ion conductor material has an ionic conductivity of between about
10
-5 S/cm and 10
-3 S/cm.
[0075] Some non-exclusive examples of electrolyte types are: solid polymer electrolytes
(SPE), such as poly(ethylene oxide) with a dissolved lithium salt; gel polymer electrolytes
(GPE), such as mixtures of poly(methyl methacrylate) and propylene carbonate with
a lithium salt; composite gel polymer electrolytes (CGPE) that are similar to GPE's
but with an addition of a second polymer such a poly(ethylene oxide), and liquid electrolytes
(LE) such as a solvent mixture of ethylene carbonate/diethyl carbonate with a lithium
salt; and composite organic-inorganic electrolytes (CE), comprising an LE with an
addition of titania, silica or other oxides. Some non-exclusive examples of lithium
salts used are LiTFSI (lithium bis(trifluoromethane) sulfonimide), LiBF
4 (lithium tetrafluoroborate), LiAsF
6 (lithium hexafluoro arsenate), LiCF
3SO
3 (lithium trifluoromethane sulfonate), and LiClO
4 (lithium perchlorate). Additional examples of suitable ion conducting layers include
silicates, silicon oxides, tungsten oxides, tantalum oxides, niobium oxides, and borates.
The silicon oxides include silicon-aluminum-oxide. These materials may be doped with
different dopants, including lithium. Lithium doped silicon oxides include lithium
silicon-aluminum-oxide. In some embodiments, the ion conducting layer comprises a
silicate-based structure. In other embodiments, suitable ion conductors particularly
adapted for lithium ion transport include, but are not limited to, lithium silicate,
lithium aluminum silicate, lithium aluminum borate, lithium aluminum fluoride, lithium
borate, lithium nitride, lithium zirconium silicate, lithium niobate, lithium borosilicate,
lithium phosphosilicate, and other such lithium-based ceramic materials, silicas,
or silicon oxides, including lithium silicon-oxide.
[0076] The thickness of the ion conducting layer 10 will vary depending on the material.
In some embodiments using an inorganic ion conductor the ion conducting layer 10 is
about 250 nm to 1 nm thick, preferably about 50 nm to 5 nm thick. In some embodiments
using an organic ion conductor, the ion conducting layer is about 100000 nm to 1000
nm thick or about 25000 nm to 10000 nm thick. The thickness of the ion conducting
layer is also substantially uniform. In one embodiment, a substantially uniform ion
conducting layer varies by not more than about +/-10% in each of the aforementioned
thickness ranges. In another embodiment, a substantially uniform ion conducting layer
varies by not more than about +/-5% in each of the aforementioned thickness ranges.
In another embodiment, a substantially uniform ion conducting layer varies by not
more than about +/-3% in each of the aforementioned thickness ranges.
[0077] Referring again to FIG. 1, substrates 24 and 25 have flat surfaces. That is, they
have a surface coincides with the tangential plane in each point. Although substrates
with flat surfaces are typically employed for electrochromic architectural windows
and many other electrochromic devices, it is contemplated that the multi-layer devices
of the present invention may have a single or even a doubly curved surface. Stated
differently, it is contemplated that each of the layers of stack 28 have a corresponding
radius of curvature. See, for example,
U.S. Patent No. 7,808,692 which is incorporated herein by reference in its entirety with respect to the definition
of single and doubly curved surfaces and methods for the preparation thereof.
[0078] FIG. 4 depicts a cross-sectional structural diagram of an electrochromic device according
to a second embodiment of the present invention. Moving outward from the center, electrochromic
device 101 comprises electrochromic electrode layer 120. On either side of electrochromic
electrode layer 120 are first and second electrically conductive layers 122, 123 which,
in turn, are arranged against outer substrates 124, 125. Elements 122, 120, and 123
are collectively referred to as an electrochromic stack 128. Electrically conductive
layer 122 is in electrical contact with a voltage source via bus bar 126 and electrically
conductive layer 123 is in electrical contact with a voltage source via bus bar 127
whereby the transmittance of electrochromic device 120 may be changed by applying
a voltage pulse to electrically conductive layers 122, 123. The pulse causes a cathodic
compound in electrochromic electrode layer 120 to undergo a reversible chemical reduction
and an anodic compound in electrochromic electrode layer 120 to undergo a reversible
chemical oxidation. Either the cathodic or anodic compound will demonstrate electrochromic
behavior such that electrochromic electrode layer 120 becomes less transmissive or
more transmissive after the pulse; in one embodiment, electrochromic device 101 has
relatively greater transmittance before the voltage pulse and lesser transmittance
after the voltage pulse or
vice versa.
[0079] Fig. 20 depicts a cross-sectional structural diagram of an electrochromic device
according to a third embodiment of the present invention. Moving outward from the
center, electrochromic device 301 comprises ion conductor layer 310. Electrochromic
electrode layer 320 is on one side of and in contact with a first surface of ion conductor
layer 310. A first electrically conductive layer 322 is in contact with electrochromic
layer 320. A second electrically conductive layer 323 is on a second surface of ion
conductor layer 310, the first and second surfaces of ion conductor layer 310 being
opposing surfaces. The first and second electrically conductive layers 322, 323 are
arranged against outer substrates 324, 325. Elements 310, 320, 322 and 323 are collectively
referred to as electrochromic stack 328. Electrically conductive layer 322 is in electrical
contact with a voltage source (not shown) via bus bar 326 and electrically conductive
layer 323 is in electrical contact with a voltage source (not shown) via bus bar 327
whereby the transmittance of electrochromic layer 320 may be changed by applying a
voltage pulse to electrically conductive layers 322, 323. Ion conductor layer 310
comprises a species that is capable of reversibly oxidizing or reducing upon the insertion
or withdrawal of electrons or ions and this species may also be electrochromically
active. The voltage pulse causes electrons and ions to move between first electrode
layer 320 and ion conducting layer 310 and, as a result, electrochromic materials
in the electrode layer 320 changes color, thereby making electrochromic device 301
less transmissive or more transmissive. In one embodiment, electrochromic device 301
has relatively greater transmittance before the voltage pulse and relatively lesser
transmittance after the voltage pulse or
vice versa.
[0080] In general, the composition and sheet resistance profiles for first and second electrically
conductive layers 122, 123, 322, 323 are as previously described in connection with
FIG. 1. Electrochromic electrode layers 120 and 320 may, for example, contain an electrochromic
material, either as a solid film or dispersed in an electrolyte, the electrochromic
material being selected from among inorganic metal oxides such as tungsten trioxide
(WO
3), nickel oxide (NiO) and titanium dioxide (TiO
2), and organic electrochromic materials including bipyridinium salt (viologen) derivatives,
N,N'-di(p-cyanophenyl) 4,4'-bipyridilium (CPQ), quinone derivatives such as anthraquinone
and azine derivatives such as phenothiazine.
[0081] In operation, to switch an electrochromic device of the present invention from a
first to a second optical state having differing transmissivities,
i.e., from a state of relatively greater transmissivity to a state of lesser transmissivity
or
vice versa, a voltage pulse is applied to the electrical contacts/bus bars on the device. Once
switched, the second optical state will persist for some time after the voltage pulse
has ended and even in the absence of any applied voltage; for example, the second
optical state will persist for at least 1 second after the voltage pulse has ended
and even in the absence of any applied voltage. By way of further example, the second
optical state may persist for at least 5 seconds after the voltage pulse has ended
and even in the absence of any applied voltage. By way of further example, the second
optical state may persist for at least 1 minute after the voltage pulse has ended
and even in the absence of any applied voltage. By way of further example, the second
optical state may persist for at least 1 hour after the voltage pulse has ended and
even in the absence of any applied voltage. The device may then be returned from the
second optical state to the first optical state by reversing the polarity and applying
a second voltage pulse and, upon being switched back, the first optical state will
persist for some time after the second pulse has ended even in the absence of any
applied voltage; for example, the first optical state will persist for at least 1
second after the voltage pulse has ended and even in the absence of any applied voltage.
By way of further example, the first optical state may persist for at least 1 minute
after the voltage pulse has ended and even in the absence of any applied voltage.
By way of further example, the first optical state may persist for at least 1 hour
after the voltage pulse has ended and even in the absence of any applied voltage.
This process of reversibly switching from a first persistent to a second persistent
optical state, and then back again, can be repeated many times and practically indefinitely.
[0082] In some embodiments the waveform of the voltage pulse may be designed so that the
local voltage across the electrochromic stack never exceeds a pre-determined level;
this may be preferred, for example, in certain electrochromic devices where excessive
voltage across the electrochromic stack can damage the device and/or induce undesirable
changes to the electrochromic materials.
[0083] Advantageously, the non-uniform sheet resistance of the first and/or second electrically
conductive layers of the multi-layer devices of the present invention may permit greater
tolerances with respect to the magnitude and/or duration of the voltage pulse. As
a result, the local voltage across the electrochromic stack may be significantly less
than the voltage applied across the entire device because of the voltage drop in the
electrically conductive layer(s). For example, in one embodiment, the applied potential
across the electrochromic stack has a magnitude of at least 2 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 3 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 4 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 5 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 6 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 7 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 8 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 9 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 10 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 11 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 12 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 13 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 14 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 15 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 16 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 18 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 20 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 22 Volts. By way of further
example, the voltage pulse may have a magnitude of at least 24 Volts. In general,
such potentials may be applied for a relatively long period of time. For example,
a potential having a magnitude of any of such values may be applied for a period of
at least 1 seconds. By way of further example, a potential having a magnitude of any
of such values may be applied for a period of at least 10 seconds. By way of further
example, a potential having a magnitude of any of such values may be applied for a
period of at least 20 seconds. By way of further example, a potential having a magnitude
of any of such values may be applied for a period of at least 40 seconds.
[0084] To illustrate for one specific exemplary embodiment, a voltage pulse of 16 volts
may be applied across an electrochromic stack incorporating two TCO electrically conductive
layers having non-uniform sheet resistance and a bus bar located at opposite perimeter
edges of the entire device. The voltage pulse rises quick to allow the local voltage
drop across the layers to quickly ramp to 1.0 volts and maintain that voltage until
the device switching approaches completeness at which point the device layers begin
to charge up and the current drops. Because of the gradient and sheet resistance in
the electrically conductive layers the voltage drop across the device is constant
across the device and in addition, there is a voltage drop across each of the electrically
conductive layers of the device. The voltage drops through the non-uniform resistivity
electrically conductive layers enables a voltage significantly larger than the maximum
operating voltage of the device stack to be applied across the entire assembly and
maintain a local voltage across the device stack below a desired value. As the device
charging takes place, the applied voltage is dropped to keep the local voltage across
the device layers at 1.0 volts. The voltage pulse will drop to a steady state value
close to 1 volt if it is desired to keep a steady state 1.0 volts across the local
device thickness or alternatively the voltage pulse will drop to zero volts if it
is desired to keep no voltage across the local device thickness in steady state.
[0085] To change the optical state of a multilayer device to an intermediate state, a voltage
pulse is applied to the electrical contacts/bus bars on the device. This shape of
this voltage pulse would typically be device specific and depend on the intermediate
state desired. The intermediate state can be defined in terms of a total charge moved,
charge state of device, or an optical measurement of the device. By using non-uniform
electron conductor layers to apply uniform local voltages across the device layers
this provides a unique advantage for rapid large area intermediate state control using
optical state feedback since a local optical measurement of the device state near
the edge will be representative of the entire device at all times (no iris effect).
Also by using non-uniform electron conductor layers to apply uniform local voltages
across the device layers this provides a unique advantage for rapid large area intermediate
state control using voltage feedback since the voltage state at the bus bars will
be representative of the entire device rather than an average across a non-uniformly
colored device (again no iris effect). In a specific example, a voltage pulse of 32
volts is applied across an electrochromic device incorporating two gradient TCO layers
and a bus bar located at opposite perimeter edges of the entire device. The voltage
pulse rises quick to allow the local voltage drop across the layers to quickly ramp
to 1.0 volts and maintain that voltage until the device reaches a desired optical
state measured with an appropriate optical sensor at which point the voltage pulse
quickly ramps down to zero or to a desired steady state voltage.
[0086] Having described the invention in detail, it will be apparent that modifications
and variations are possible without departing the scope of the invention defined in
the appended claims. Furthermore, it should be appreciated that all examples in the
present disclosure are provided as non-limiting examples.
EXAMPLES
[0087] The following non-limiting examples are provided to further illustrate the present
invention. It should be appreciated by those of skill in the art that the techniques
disclosed in the examples that follow represent approaches the inventors have found
function well in the practice of the invention, and thus can be considered to constitute
examples of modes for its practice. However, those of skill in the art should, in
light of the present disclosure, appreciate that many changes can be made in the specific
embodiments that are disclosed and still obtain a like or similar result without departing
from the spirit and scope of the invention.
EXAMPLE 1: IRIS EFFECT SWITCHING
[0088] A 1-D lumped element circuit model has been used to simulate the dynamic behavior
of an electrochromic type device using component values appropriate to capture the
switching dynamics of a large area device. The lumped element model shown in FIG.
5 is based on a paper by
Skrayabin et. al. (Electrochimica Acta 44 (1999) 3203-3209). The electrochromic device is locally modeled by a parallel resistor and non-linear
capacitor and the electrically conducting layer is locally modeled as a resistor.
A network of these devices as shown in FIG. 5 models the behavior of a large area
electrochromic device. A low resistance resistor between the device and the power
supply simulates the contact resistance between the power supply and the device. FIG.
6 shows the applied voltage, a 1.1 volt step function. The resultant current flow
is shown in FIG. 7; it rises rapidly to a maximum value and then decreases as the
device switching takes place. FIG. 8 shows the voltage drop across the electrochromic
device near the edge of the device, part way toward the center, and near the center
of the device from both sides of the device (six traces total). What is seen is that
the edge of the device switches relatively slowly and moving towards the center of
the device the switching occurs even more slowly. The slower switching of the center
of the device relative to the edge is the well understood characteristic of large
area devices referred to as the iris effect.
[0089] The switching speed of this entire device can be increased by applying a more complex
voltage waveform. Such a waveform along with its effect on the current and effect
on switching dynamics is shown in FIGS. 9-11. The applied voltage pulse was selected
to ramp up the voltage near the edge to a maximum, not to exceed 1.0 volts. This required
that the voltage waveform quickly ramp up and then decrease the voltage in time as
needed to keep the voltage across the device below 1.0 volts. This waveform is shown
in FIG. 9. The current flowing out of the power supply is shown in FIG. 10 and shows
a sharp initial current increase followed by a decreasing current over time following
the decrease in applied voltage. FIG. 11 shows the voltage drop across the device
near the edge of the device, part way towards the center of the device, and near the
middle of the device from both contacts (6 traces in total). It can be seen that the
device in this case switches near the edge of the device much faster than in the previous
example, where the applied voltage was a step function. Near the center of the device
the switching is still slow and while the whole device switches faster than in the
previous case, the iris effect may be exacerbated as the voltage difference between
the edge and the center is larger during part of the switching. Note that the switching
is symmetric such that the curves corresponding to points located symmetrically opposite
on the device switch identically and overlap. This iris effect can be reduced or eliminated
by adjusting the sheet resistance distribution in the electron conductor layers of
the multi-layer device as shown in the next example.
EXAMPLE 2: UNIFORM SWITCHING
[0090] The 1-D circuit model shown in FIG. 12 embodies a constant gradient in sheet resistance
in each of the electrically conducting layers. These are arranged such that the sheet
resistance is lowest near the connection the power supply and highest at the opposite
end of the device. One polarity of the power supply is applied to one electrically
conducting layer and the other polarity of the power supply is applied to the opposing
electrically conducting layer and at the opposite sides of the device. With this arrangement
there is no iris effect and switching behavior is qualitatively different - providing
both uniform switching across the entire device and much faster switching of the entire
device. This switching behavior is shown in FIGS. 13-15. FIG. 13 shows the applied
voltage waveform. This waveform was selected to limit the voltage across the device
to always be below a desired threshold (in this example 1.0 volts). The resultant
waveform is a voltage pulse with a fast rising leading edge and a slower falling edge
selected to keep the voltage across the device below but near the desired threshold
voltage. FIG. 14 shows the current flowing through the device as a function of time,
the current ramps up quickly and has a waveform similar in shape to that of the applied
voltage pulse. FIG. 15 shows the voltage drop across the electrochromic device at
the edge of the device near the power supply contact and near the center of the device.
As can be seen in this plot, the voltage profile across the device is the same at
all locations. The result is that significant current can be driven through the device
in a relatively short period of time while the voltage across the device is low and
the same everywhere. Such a non-uniform sheet resistance in the electrically conducting
layers can allow large area electrochromic devices to switch with dynamics similar
to those of small area devices.
EXAMPLE 3: DIRECTIONAL SWITCHING
[0091] The lumped element model in FIG. 16 is an example of a configuration that provides
a controlled switching profile in an electrochromic device. In this case, the device
will switch from left to right. The electrically conducting layers are asymmetric.
The top electrically conducting layer is a layer with sheet resistance of 5 Ω/□ at
the left side and linearly increasing to 50 Ω/□ at the right side of this layer. The
bottom electrically conducting layer is a layer with sheet resistance of 30 Ω/□ at
the left side and linearly decreasing to 3 Ω/□ at the right side of the layer. FIG.
17 shows the applied voltage waveform to product a rapidly rising voltage at the left
side of the device while keeping this voltage across the device below 1.0 volts. FIG.
18 shows the corresponding current through the device which initially rapidly increases
then quickly falls as the device switches. FIG. 19 shows the voltage across the device
at six location from left to right. As can be seen, the voltage increases and approaches
1.0V at the far left side the fastest and at each point further right the voltage
across the device increases and approaches 1.0V more slowly. This will result in a
device that will switch from left to right in a pre-determined manner. This behavior
can be controlled at window sizes that would exhibit an iris effect with a given constant
sheet resistance in the electrically conducting layers. In addition the rate at which
the apparent velocity of switching occurs from left to right can be controlled by
the difference between the sheet resistance profiles in the electrically conducting
layers. For example, if the lower electrically conducting layer in Example 3 was a
layer with sheet resistance of 40 Ω/□ at the left side and linearly decreasing to
4 Ω/□ at the right side of the layer then the switching of the device in this case
would be much faster from left to right. In the limiting case that that the sheet
resistance profiles are linear and identical in opposing directions then the device
will switch uniformly as demonstrated in Example 2.
EXAMPLE 4 AND COMPARATIVE EXAMPLE 4A
[0092] All substrates for Example 4 and Comparative Example 4A (and Examples 5-7 and comparative
examples), were 9x13.7 cm in dimension and between 2.3 and 4 mm thick.
[0093] Devices containing a single electrochromic electrode layer and a single ion conductor
layer positioned between two electrically conductive layers located between two outer
substrates of glass were prepared for the example and comparative example. Electrically
conductive layers were tin doped indium oxide (ITO) transparent conductive oxide (TCO)
layers sputter-coated on float glass substrates. Comparative Example 4A used ITO coated
substrates with a uniform sheet resistance of 65 Ω/□. Example 4 used ITO coated substrate
with a linear increase in sheet resistance from 70-400 Ω/□. The sheet resistance increased
linearly in the 13.7 cm direction (
i.e., a constant sheet resistance gradient) and was approximately uniform in the 9 cm
direction. The ITO substrates were custom prepared for the work by sputtering onto
bare float glass substrates. The procedure for fabrication of the devices is detailed
below.
[0094] The sheet resistance of the ITO coated substrates was measured using a 4-point probe
measurement tool. Sheet resistance measurements on the gradient resistance ITO substrates
were made on at least at five equally spaced locations placed on a straight line with
the line running perpendicular to the 9 cm sides of the substrate and with the measured
locations covering the majority of the sheet resistance gradient.
[0095] A tungsten oxide precursor was prepared as follows. In a 0°C ice bath, a 2 L flask
was charged with 40 mL water and fitted with a stir bar. Then 800 mL of a 50:50 solution
of aqueous hydrogen peroxide (30 wt. % H
2O
2) and glacial acetic acid was added and stirred 30 minutes to equilibrate to the ice
bath temperature. To the cold mixture, 65 g of tungsten metal was added and stirred
to react for 24 hours. The resulting solution was filtered through coarse (Whatman
54) and then fine (Whatman 42) filter paper to yield a clear, slightly yellow filtrate.
The filtrate was then refluxed 18 hours at 55°C and refiltered through fine (Whatman
42) filter paper, then dried under vacuum (using a water aspirator) at 65°C to recover
a powdered tungsten peroxy acid ester product.
[0096] The coating solution was prepared by dissolving 18 g of the solid tungsten peroxy
acid precursor, 0.668g lithium methoxide, and 2.367 g oxalic acid dehydrate in 60
mL anhydrous ethanol under an argon atmosphere in a glove box.
[0097] The coating solution was spin-coated onto the two TCO types (uniform sheet resistance
and gradient sheet resistance).
[0098] Following coating, a strip of the coated film was removed from all sides of the substrate
using water. This exposed the underlying TCO for electrical contacts and better adhesion.
The films were processed with the following program in a humidity chamber.
Step |
Temperature °C |
Relative Humidity (%) |
Time (min) |
1 |
26 |
40 |
5 |
2 |
30 |
80 |
10 |
3 |
45 |
70 |
15 |
4 |
60 |
65 |
15 |
5 |
90 |
10 |
10 |
6 |
105 |
1 |
10 |
7 |
25 |
25 |
19 |
[0099] After removal from the humidity chamber, the films were processed in an oven in air
with the following program to produce a tungsten oxide film.
Step |
Temperature °C |
Time (min) |
1 |
Ambient |
0 |
2 |
Ramp to 240 |
60 |
3 |
240 |
60 |
4 |
Ambient |
60 |
[0100] Final thickness was measured by a contact profilometer to be approximately 300 nm.
[0101] Two holes 4 mm in diameter were drilled into opposite corners of a set of ITO substrates
(one uniform sheet resistance ITO and one gradient sheet resistance ITO). The devices
were then constructed by hermetically sealing matching substrates together using thermal-set
epoxy around the outside edge with the conductive surfaces facing inward (e.g., two
uniform sheet resistance ITO substrates were used in a single device while two gradient
sheet resistance ITO substrates were used in another device). A fixed gap width of
210 µm was set by mixing glass beads with a known diameter into the epoxy. The substrates
were shifted relative to each other to produce an overlap of approximately 0.5 cm
in all directions to permit electrical connections and electrical measurements. Busbars
for electrical contact were soldered onto the overlapping sections on the short sides
of the device (
i.e., 9 cm sides). The gradient ITO device was assembled with the gradients opposing
each other and with their low sheet resistance sides serving as the busbar area for
contacts (
i.e., the low sheet resistance side of each substrate was aligned to face the high sheet
resistance side of the other and both low sides positioned to be exposed.)
[0102] The prepared devices were filled through the drilled holes with an ion conductor
solution of 0.5 M lithium triflate and 0.05 M ferrocene in anhydrous propylene carbonate.
The holes were then sealed. In these devices the ferrocene in the ion conductor layer
acts as a species capable of reversibly oxidizing and reducing upon the insertion
or withdraw of electrons.
[0103] Analysis and characterization of the completed devices was carried out using a custom
lab instrument. The instrument permitted simultaneous control of the voltage source,
measurement of transmission across the electromagnetic spectrum at various points
in the device, and voltage potential across the electrochemical stack at various points.
This allows full characterization of the device and links voltage potential in the
electrochromic stack at a particular point in the device to electromagnetic transmission
at that same point. For example, a device could be characterized with a pre-set voltage
pulse profile and simple measurement of voltage and optical data. Additionally, the
device could be characterized with the voltage pulse adjusting to maintain a target
voltage potential in the electrochromic stack.
[0104] The devices of Comparative Example 4A and Example 4 were characterized. Data showing
variations in voltage and transmission values are presented below. The "Iris" value
is the maximum difference in transmission at 550 nm between an area near the edge
and the center of the device measured while switching the device from bleached to
colored states. The Maximum Voltage Δ is the maximum difference in voltage potential
across the electrochromic stack near the edge and the center of the device while switching
the device from bleached to colored states. The source voltage was automatically adjusted
to maintain 1.2 volts across the electrochromic stack at the edge of the device. Total
time to steady state was approximately 150 seconds in each case.
|
Maximum Voltage Δ |
Maximum Iris Value (ΔT at 550 nm) |
Comparative Example 4 |
0.64 V |
31% |
Example 4 |
0.25 V |
6% |
EXAMPLE 5 AND COMPARATIVE EXAMPLE 5A
[0105] Devices comprising two electrochromic electrode layers, positioned on each side of
a single ion conductor layer with each electrochromic electrode layer positioned against
an electrically conductive TCO layer and with each TCO layer arranged against an outer
substrate of glass were prepared for the example and comparative example. Comparative
Example 5A used ITO coated substrates with a uniform sheet resistance of approximately
220 Ω/□. Example 5 used ITO coated substrates with a constant gradient in sheet resistance
from approximately 100-500 Ω/□. The gradient device was constructed with the substrates
oriented as in Example 4. The ITO was custom sputter deposited for the project and
then thermally processed to increase its sheet resistance. Sheet resistance measurements
were taken on deposited electrode films following thermal processing and just prior
to insertion into a final device.
[0106] The sheet resistance of the ITO coated substrates was measured using a 4-point probe
measurement tool. Sheet resistance measurements on the uniform ITO coated substrates
were made at several points on the film. Sheet resistance measurements on the gradient
sheet resistance ITO substrates were made on at least five equally spaced locations
on a straight line with the line running perpendicular and between the two 9 cm sides
of the substrate. It was observed that the sheet resistance of the ITO would vary
due to thermal treatment and application of an electrode film. A correction factor
was applied to the sheet resistance measurements after thermal treatment or application
of an electrode film. The correction factor was calculated by measuring the overall
sheet resistance of the substrate between two points placed at the mid-point of each
9 cm side and offset from the edge by approximately 0.5 cm and ensuring measurement
on exposed TCO. The correction factor was then the ratio of this overall sheet resistance
of the substrate from before and after the treatment. For example, if this sheet resistance
increased from 100 Ω to 150 Ω due to a thermal treatment and the original measured
sheet resistance in Ω/□ was 200 Ω/□ then the reported sheet resistance in Ω/sq after
thermal treatment was 300 Ω/□.
[0107] Tungsten oxide films were prepared as in Example 4 on the two substrate types (
i.e., one uniform sheet resistance and one gradient sheet resistance substrate). The
tungsten oxide films served as the first electrode layers.
[0108] Complimentary vanadium oxide xerogel films were prepared on the two substrate types.
Two holes 4 mm in diameter were drilled into opposite corners of this set before coating.
The vanadium oxide films served as the second electrode layer.
[0109] The vanadium oxide xerogel coating proceeds by acidification of LiVO
3 by cation exchange followed promptly by spin coating before gelation of the resulting
vanadic acid can occur. The procedure for the coating solution is as follows.
[0110] A 2 M LiVO
3 precursor solution was prepared by dissolving 8.08 g LiVO
3 in 34 mL 40%vol aqueous ethanol by stirring at 60°C for 1 hour. The cloudy solution
was filtered (Whatman 40), and the filter rinsed with 40% ethanol. The filtrate was
diluted to 40 mL and shaken to mix yielding a slightly yellow, viscous 2 M LiVO
3 solution.
[0111] The flash ion exchange columns were prepared by packing 2 mL (3.4 meq) of Dowex WX8
100-200 mesh cation exchange resin (proton form) into a 3 mL syringe fitted with a
0.2 micron PTFE Acrodisk filter to retain the resin beads. The columns were rinsed
twice with water and then drained. One milliliter of the LiVO
3 solution was added to a packed syringe, which was shaken ten seconds to mix into
the resin. The "column" was eluted by depressing the syringe plunger and the bright
orange vanadic acid solution was immediately refiltered (0.2 micron PTFE Acrodisk)
onto the substrate and spun to form the coating. Following coating, a strip of the
coated film was removed from all sides of the substrate using a water treatment. This
exposed the underlying TCO for electrical contacts and better adhesion.
[0112] The resulting films were thermally processed using the following recipe to produce
a vanadium oxide film.
Step # |
Procedure |
Time |
1 |
Heat 25°C to 240°C |
60 minutes |
2 |
Hold at 240°C |
60 minutes |
3 |
Cool 240°C to 40°C |
120 minutes |
[0113] Final thickness was measured by a contact profilometer to be approximately 100 nm.
[0114] The vanadium oxide films were lithiated in a glove box using a lithium metal counter-electrode
and a solution of 1 M lithium perchlorate in propylene carbonate. A two-step procedure
involving oxidation to 3.8V followed by reduction at 2.4 V was performed with the
voltages quoted versus reference lithium metal. Lithiation was performed to put the
vanadium oxide into a state of reduction that allows it to serve as the counter-electrode
to the tungsten oxide films.
[0115] The devices were then constructed by hermitically sealing matching substrates together
using an acrylic adhesive tape with the conductive surfaces facing inward. A fixed
gap width of 500 µm was set by the adhesive tape. Acrylic adhesive tape was used for
rapid device creation. The substrates were shifted relative to each other to produce
an overlap of approximately 0.5 cm in all directions to permit electrical connections
and measurements. The gradient device was assembled as in Example 4 with the low sheet
resistance sides exposed for electrical contact.
[0116] The prepared devices were filled through the drilled holes with an electrolyte solution
of 1.5 M Lithium Bis(trifluoromethanesulfonyl)imide in anhydrous propylene carbonate.
The holes were then sealed.
[0117] The Example 5 and Comparative Example 5A devices were analyzed with the custom setup
described in Example 4. The results are shown below
Source voltage |
Switching time (bleached to colored) |
Maximum Voltage Δ |
Iris Value (ΔT at 550 nm) |
Comparative Example 5A. Electrochemical stack at edge of device controlled to 1.2
V |
150 seconds |
1.4 V |
17% |
Example 5. Electrochemical stack at edge of device controlled to 1.2 V |
<100 Seconds |
0.3 V |
6% |
[0118] As demonstrated by the results, the device of Example 5 significantly mitigated the
Iris value while achieving a faster switching speed than the device of Comparative
Example 5A.
EXAMPLE 6
[0119] A device was prepared containing two electrochromic electrode layers, positioned
on each side of a single ion conductor layer with each electrochromic electrode layer
positioned against an electrically conductive TCO layer and with each TCO layer arranged
against an outer substrate of glass. The device of this example 6 used TEC 70 substrates
(Pilkington) with two laser scribed patterns. TEC glass is commercially available
fluorine doped tin oxide (FTO) where the number in the name indicates the sheet resistance
in Ω/□. FTO is a TCO. The laser scribed patterns increase and modulate the sheet resistance
of the TCO. The first TEC substrate had a laser pattern that simulated a uniform sheet
resistance of 250 Ω/□. The second TEC substrate had a laser scribe pattern that simulated
a linear increase in sheet resistance from 170-1500 Ω/□ substrate.
[0120] The sheet resistance of scribed TEC glass substrates was calculated by measuring
the sheet resistance between two points spaced one cm apart on the substrate. The
same measurement was performed on a set of un-scribed TEC glass with a known sheet
resistance value in Ω/□. From the un-scribed TEC measurements a calibration curve
was calculated relating Ω/□ to the 2-point sheet resistance value. A sheet resistance
value in Ω/□ was then calculated for each measurement on the scribed TEC glass substrates.
The second TEC glass substrate sheet resistance profile was measured by taking individual
measurements at 1 cm intervals in a straight line between and perpendicular to the
two 9 cm sides of the substrate.
[0121] The device should be compared with Example 3. Example 3 describes a lumped element
model of an electrochromic device with a directional switch. This directional switch
is achieved in Example 3 by an asymmetry in the electrically conductive layer (
e.g., the TCO). The device of Example 6 has an asymmetry in the two electrically conductive
layers and was expected to show a directional switch where the device switches faster
on the low sheet resistance side of the second TEC substrate and slower on the high
sheet resistance side of the second TEC substrate.
[0122] The device was constructed using the procedure described below.
[0123] The tungsten oxide film was prepared as in Example 4 on the second TEC substrate
(with gradient sheet resistance). The tungsten oxide film served as the first electrode
layer.
[0124] A complementary vanadium oxide film was prepared on the first TEC substrate (uniform
sheet resistance). The vanadium oxide film served as the second electrode layer. Two
holes approximately 4 mm in diameter were drilled into opposite corners of the uniform
sheet resistance substrate before coating. The coating solution was prepared according
to the following recipe.
[0125] A solution of LiVO
3 was prepared by dissolving the solid in 5%wt solution in water at 60 °C, followed
by filtration through Whatman 40 paper. The vanadate species were protonated to "vanadic
acid" by running this 5%wt solution of LiVO
3 dropwise through an ion exchange column packed with at least 20 equivalents of Dowex
Monosphere 650C in H
+ form, eluting with additional deionized water until a pale yellow endpoint. The eluted
vanadic acid was allowed to stand overnight, after which it was sonicated to disperse
any solids that had formed.
[0126] Six equivalents of triethylamine were added to the vanadic acid and the mixture was
sonicated at 40-50°C for one hour to form a colorless, slightly turbid. This solution
was evaporated under reduced pressure at up to 55°C to yield a yellow viscous liquid.
This was dissolved in ethanol or 2-methoxyethanol to between 0.4 M vanadium and 1.2
M vanadium to yield a final coating solution.
[0127] The coating solution was spin-coated onto the substrate. Following coating, a strip
of the coated film was removed from all sides of the substrate using a water treatment.
This exposed the underlying TCO for electrical contacts and better adhesion. The film
was thermally processed using the following recipe in air to produce a vanadium oxide
film.
Step # |
Procedure |
Time |
1 |
Heat 25°C to 350°C |
60 minutes |
2 |
Hold at 350°C |
60 minutes |
3 |
Cool 350°C to 40°C |
120 minutes |
[0128] Final thickness was measured by a contact profilometer to be approximately 200 nm.
[0129] The vanadium oxide film was lithiated in a glove box using a lithium metal counterelectrode
and a 1 M solution of lithium perchlorate in propylene carbonate. The voltage during
lithiation was 2.7 to 2.9 volts versus lithium metal. Lithiation was performed to
put the vanadium oxide into a state of reduction that allows it to serve as the counter-electrode
to the tungsten oxide film.
[0130] The devices were then constructed by hermitically sealing matching substrates together
using thermal setting epoxy around the outside edge with the conductive surfaces facing
inward. A fixed gap width of 210 µm was set by mixing glass beads of a known diameter
into the epoxy. The substrates were shifted relative to each other to produce an overlap
of approximately 0.5 cm in all directions to permit electrical connections and measurements.
The device was constructed with the gradient substrate oriented with the low sheet
resistance side exposed for electrical connection.
[0131] The prepared devices were hydrated in a humidity chamber at 25% relative humidity
at 25°C for 2 hours. The prepared devices were then filled through the drilled holes
with an electrolyte solution of 1.5 M Lithium Bis(trifluoromethanesulfonyl)imide in
anhydrous propylene carbonate. The holes were then sealed.
[0132] The device of Example 6 was characterized and demonstrated a pronounced directional
change effect where the device switched from bleached to colored states substantially
faster on the low sheet resistance side of the second TEC substrate than the high
sheet resistance side of the second TEC substrate. The difference in transmission
exceeded 25% during coloration. This directional change qualitatively agreed with
the prediction made in Example 3.
EXAMPLE 7 AND COMPARATIVE EXAMPLE 7A
[0133] Devices were made containing two electrode one of which being electrochromic, positioned
on each side of a single ion conductor layer with each electrode layer positioned
against an electrically conductive TCO layer and with each TCO layer arranged against
an outer substrate of glass. The device of Comparative Example 7A used TEC 70 substrates
(Pilkington) with a laser scribed pattern to simulate 250 Ω/□ sheet resistance. The
laser scribed patterns increase and modulate the sheet resistance of the TCO. The
device of Example 7 used TEC 70 substrates with a laser scribed pattern that simulated
a 70-250 Ω/□ substrate. Sheet resistance values were calculated as in Example 6. The
device was constructed with the substrates oriented with opposing sheet resistance
gradients as in Example 4. All devices were constructed using the procedure described
below.
[0134] A 20wt% colloidal dispersion of cerium oxide coating solution in an aqueous solution
(Alfa Aesar) was spin-coated onto a set of the laser scribed FTO substrates. Following
spin-coating, a strip of the cerium oxide film was removed from all sides using an
acetic acid solution (aq., 2.5wt%). The film was thermally processed for one hour
at 240 °C in air.
[0135] Final thickness was measured by profilometry to be approximately 350 nm.
[0136] The cerium oxide films served as the first electrode layer.
[0137] Complementary vanadium oxide films were prepared on the same set of substrates. The
vanadium oxide films served as the second electrode layer and is electrochromic. Two
holes 4 mm in diameter were drilled into the corners of this set before coating. The
vanadium solution was prepared according to the following procedure.
[0138] A 2 M LiVO
3 precursor solution was prepared by dissolving 8.08 g LiVO
3 in 34 mL 40%vol aqueous ethanol by stirring at 60°C for 1 hour. The cloudy solution
was filtered (Whatman 40), and the filter rinsed with 40% ethanol. The filtrate was
diluted to 40 mL and shaken to mix yielding a slightly yellow, viscous 2 M LiVO
3 solution.
[0139] Twenty milliliters of this LiVO
3 solution was acidified by the addition of between 4.5 and 6 g Dowex Monosphere 650C
cation exchange resin (proton form) under vigorous stirring. The resulting bright
orange mixture was filtered through filter paper (Whatman 40) and then diluted with
6.6 mL water to yield the final coating solution.
[0140] The coated films were thermally processed one hour at 240°C in air to yield a vanadium
oxide film. Final thickness was measured by a contact profilometer to be approximately
150 nm.
[0141] The vanadium oxide films were lithiated in a glove box using a lithium metal counterelectrode
and a solution of 1 M lithium perchlorate in propylene carbonate. A two-step procedure
involving oxidation to 3.8V followed by reduction at 2.4 V was performed with the
voltages quoted versus reference lithium metal. Lithiation was performed to put the
vanadium oxide into a state of reduction that allows it to serve as the counter-electrode
to the cerium oxide films.
[0142] The devices were then constructed by hermitically sealing matching substrates together
using acrylic adhesive tape around the outside edge with the conductive surfaces facing
inward. A fixed gap width of 500 µm was set by the adhesive tape. The substrates were
shifted relative to each other to produce an overlap of approximately 0.5 cm in all
directions to permit electrical connections and measurements. The gradient device
was assembled as in Example 4 with the low sheet resistance sides exposed for electrical
contact.
[0143] The prepared devices were then filled through the drilled holes with an electrolyte
solution of 1.5 M Lithium Bis(trifluoromethanesulfonyl)imide in anhydrous propylene
carbonate. The holes were then sealed.
[0144] The Iris Value for these devices was measured at 450 nm. This wavelength was used
as it showed a larger change in transmittance between the bleached and colored states
than 550 nm.
Source voltage |
Switching time (bleached to colored) |
Maximum Voltage Δ |
Iris Value (ΔT at 450 nm) |
Comparative Example 7A. Electrochemical stack at edge of device controlled to 2 V. |
>180 seconds |
1.6 V |
6% |
Example 7. Electrochemical stack at edge of device controlled to 2 V. |
75 seconds |
0.3 V |
3% |
[0145] The gradient device achieved more uniform switching and significantly faster switching
speed.
Aspects of the Invention
[0146]
- 1. A multi-layer device comprising a first substrate and a first electrically conductive
layer on a surface thereof, the first electrically conductive layer being transmissive
to electromagnetic radiation having a wavelength in the range of infrared to ultraviolet
and having a sheet resistance, Rs, to the flow of electrical current through the first electrically conductive layer
that varies as a function of position in the first electrically conductive layer wherein
the ratio of the value of maximum sheet resistance, Rmax, to the value of minimum sheet resistance, Rmin, in the first electrically conductive layer is at least 2.
- 2. The multi-layer device of aspect 1 wherein the ratio of the average sheet resistance
in a first region of the first electrically conductive layer circumscribed by a first
convex polygon to the average sheet resistance in a second region of the first electrically
conductive layer circumscribed by a second convex polygon is at least 2, the first
and second regions circumscribed by the first and second convex polygons, respectively,
each comprising at least 25% of the surface area of the first electrically conductive
layer.
- 3. The multi-layer device of aspect 1 or 2 wherein the ratio of the average sheet
resistance in a first region of the first electrically conductive layer, R1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R2avg, is at least 1.25, the ratio of the average sheet resistance in the second region
of the first electrically conductive layer, R2avg, to the average sheet resistance in a third region of the first electrically conductive
layer, R3avg, is at least 1.25, the ratio of the average sheet resistance in the third region
of the first electrically conductive layer, R3avg, to the average sheet resistance in a fourth region of the first electrically conductive
layer, R4avg, is at least 1.25, wherein the first region is contiguous with the second region,
the second region is contiguous with the third region, the third region is contiguous
with the fourth region, each of the regions is circumscribed by a convex polygon,
and each comprises at least 10% of the surface area of the first electrically conductive
layer.
- 4. The multi-layer device of any of aspects 1-3 wherein the first electrically conductive
layer has a spatially varying sheet resistance, Rs, that varies as a function of position in the first electrically conductive layer,
a contour map of the sheet resistance, Rs, as a function of position within the first electrically conductive layer contains
a set of isoresistance lines and a set of resistance gradient lines normal to the
isoresistance lines, and the sheet resistance along a gradient line in the set generally
increases, generally decreases, generally increases until it reaches a maximum and
then generally decreases, or generally decreases until it reaches a minimum and then
generally increases.
- 5. The multi-layer device of any of aspects 1-4 wherein the first electrode layer
is graded in composition or thickness.
- 6. The multi-layer device of any of aspects 1-5 wherein the first substrate is transparent
to electromagnetic radiation having a wavelength in the range of infrared to ultraviolet.
- 7. The multi-layer device of any of aspects 1-6, the multi-layer device further comprising
a first electrode layer on a surface of the first electrically conductive layer, the
first electrically conductive layer being between the first electrode layer and the
first substrate.
- 8. The multi-layer device of aspect 7 wherein the first electrode layer comprises
an electrochromic material.
- 9. The multi-layer device of aspect 7 wherein the first electrode layer comprises
an anodic species and a cathodic species, at least one of the anodic species and the
cathodic species being an electrochromic material.
- 10. The multi-layer device of any of aspects 7-9, the multi-layer device further comprising
a second electrically conductive layer, the first electrode layer being transparent
to electromagnetic radiation having a wavelength in the range of infrared to ultraviolet
and located between the first and second electrically conductive layers, the second
electrically conductive layer having a sheet resistance, Rs, to the flow of electrical current through the second electrically conductive layer
that varies as a function of position in the first electrically conductive layer wherein
the ratio of the value of maximum sheet resistance, Rmax, to the value of minimum sheet resistance, Rmin, in the second electrically conductive layer is at least 2.
- 11. The multi-layer device of aspect 10 wherein the ratio of the average sheet resistance
in a first region of the second electrically conductive layer circumscribed by a first
convex polygon to the average sheet resistance in a second region of the second conductive
layer circumscribed by a second convex polygon is at least 2, the first and second
regions circumscribed by the first and second convex polygons, respectively, each
comprising at least 25% of the surface area of the second electrically conductive
layer.
- 12. The multi-layer device of aspect 10 or 11 wherein the ratio of the average sheet
resistance in a first region of the second electrically conductive layer, R1avg, to the average sheet resistance in a second region of the second electrically conductive
layer, R2avg, is at least 1.25, the ratio of the average sheet resistance in the second region
of the second electrically conductive layer, R2avg, to the average sheet resistance in a third region of the second electrically conductive
layer, R3avg, is at least 1.25, the ratio of the average sheet resistance in the third region
of the second electrically conductive layer, R3avg, to the average sheet resistance in a fourth region of the second electrically conductive
layer, R4avg, is at least 1.25, wherein the first region is contiguous with the second region,
the second region is contiguous with the third region, the third region is contiguous
with the fourth region, each of the regions is circumscribed by a convex polygon,
and each comprises at least 10% of the surface area of the second electrically conductive
layer.
- 13. The multi-layer device of any of aspects 10-12 wherein the second electrically
conductive layer has a spatially varying sheet resistance, Rs, that varies as a function of position in the second electrically conductive layer,
a contour map of the sheet resistance, Rs, as a function of position within the second electrically conductive layer contains
a set of isoresistance lines and a set of resistance gradient lines normal to the
isoresistance lines, and the sheet resistance along a gradient line in the set generally
increases, generally decreases, generally increases until it reaches a maximum and
then generally decreases, or generally decreases until it reaches a minimum and then
generally increases.
- 14. The multi-layer device of any of aspects 10-13 wherein (a) the first electrically
conductive layer comprises a region A and a region B wherein region A and region B
each comprise at least 25% of the surface area of the first electrically conductive
layer, are each circumscribed by a convex polygon and are mutually exclusive, (b)
a projection of region A onto the second electrically conductive layer defines a region
A1 circumscribed by a convex polygon in the second electrically conductive layer comprising
at least 25% of the surface area of the second electrically conductive, (c) a projection
of region B onto the second electrically conductive layer defines a region B1 circumscribed by a convex polygon in the second electrically conductive layer comprising
at least 25% of the surface area of the second electrically conductive, (d) the first
electrically conductive layer has an average sheet resistance in region A corresponding
to RAavg and an average sheet resistance in region B corresponding to RBavg (e) the second electrically conductive layer has an average sheet resistance in region
A1 corresponding to RA1avg and an average sheet resistance in region B corresponding to RB1avg, (f) the ratio of RAavg to RBavg or the ratio of RB1avg to RA1avg is at least 1.5 and (g) the ratio of (RAavg/RA1avg) to (RBavg/RB1avg) is at least 1.5.
- 15. The multi-layer device of any of aspects 7-14, the multi-layer device further
comprising an ion conducting layer, the first electrode layer being between the ion
conducting layer and the first electrically conductive layer, the ion conducting layer
being a dielectric material having an ionic conductivity for carrier ions of at least
10-7 Siemens/cm at 25 °C.
- 16. The multi-layer device of aspect 15, the multi-layer device further comprising
a second electrode layer, the ion conducting layer being between the first and second
electrode layers.
- 17. The multi-layer device of aspect 16 wherein the second electrode layer comprises
an electrochromic material.
- 18. The multi-layer device of any of aspects 7-17, the multi-layer device further
comprising a second substrate, the second electrically conductive layer being between
the second substrate and the first electrically conductive layer.
- 19. The multi-layer device of aspect 18 wherein the second substrate is transparent
to electromagnetic radiation having a wavelength in the range of infrared to ultraviolet.
- 20. The multi-layer device of any of aspects 1-19 wherein the first substrate has
an inner surface facing the first electrically conductive layer, the surface area
of the inner surface of the first substrate being at least 0.1 meter2.
- 21. An electrochromic device comprising a first substrate, a first electrically conductive
layer, a first electrode layer, a second electrically conductive layer and a second
substrate, the first and second electrically conductive layers each having a sheet
resistance, Rs, to the flow of electrical current through the first and second electrically conductive
layers that varies as a function of position in the first and second electrically
conductive layers, respectively, wherein the ratio of the value of maximum sheet resistance,
Rmax, to the value of minimum sheet resistance, Rmin, in the first electrically conductive layer is at least 2 and the ratio of the value
of maximum sheet resistance, Rmax, to the value of minimum sheet resistance, Rmin, in the second electrically conductive layer is at least 2, the first substrate and
the first electrically conductive layer being transmissive to electromagnetic radiation
having a wavelength in the range of infrared to ultraviolet.
- 22. The electrochromic device of 21 wherein (i) the ratio of the average sheet resistance
in a first region of the first electrically conductive layer circumscribed by a first
convex polygon to the average sheet resistance in a second region of the first electrically
conductive layer circumscribed by a second convex polygon is at least 2, the first
and second regions of the first electrically conductive layer each comprising at least
25% of the surface area of the first electrically conductive layer and (ii) the ratio
of the average sheet resistance in a first region of the second electrically conductive
layer circumscribed by a first convex polygon to the average sheet resistance in a
second region of the second electrically conductive layer circumscribed by a second
convex polygon is at least 2, the first and second regions of the second electrically
conductive layer each comprising at least 25% of the surface area of the second electrically
conductive layer.
- 23. The electrochromic device of aspect 21 or 22 wherein the first electrically conductive
layer has a spatially varying sheet resistance, Rs, that varies as a function of position in the first electrically conductive layer,
a contour map of the sheet resistance, Rs, as a function of position within the first electrically conductive layer contains
a set of isoresistance lines and a set of resistance gradient lines normal to the
isoresistance lines, and the resistance along a gradient line in the set generally
increases, generally decreases, generally increases until it reaches a maximum and
then generally decreases, or generally decreases until it reaches a minimum and then
generally increases.
- 24. The electrochromic device of aspect 23 wherein the second electrically conductive
layer has a spatially varying sheet resistance, Rs, that varies as a function of position in the second electrically conductive layer,
a contour map of the sheet resistance, Rs, as a function of position within the second electrically conductive layer contains
a set of isoresistance lines and a set of resistance gradient lines normal to the
isoresistance lines, and the resistance along a gradient line in the set generally
increases, generally decreases, generally increases until it reaches a maximum and
then generally decreases, or generally decreases until it reaches a minimum and then
generally increases.
- 25. The electrochromic device of aspect 23 wherein (i) the first electrically conductive
layer has a spatially varying sheet resistance, Rs, that varies as a function of position in the first electrically conductive layer,
(ii) a contour map of the sheet resistance, Rs, as a function of position within the first electrically conductive layer contains
a set of isoresistance lines and a set of resistance gradient lines normal to the
isoresistance lines, and (iii) a projection of a line segment having a length of at
least 1 cm of one of the gradient lines onto the second electrically conductive layer
defines a complementary line segment in the second electrically conductive layer wherein
(a) the average value of the slope of the sheet resistance of the first electrically
conductive layer over the gradient line segment, S1avg, is a positive or negative value, and (b) the average value of the slope of the sheet
resistance of the second electrically conductive layer over the complementary line
segment, S2avg, is zero or is opposite in sign to S1avg.
- 26. The electrochromic device of any of aspects 21-25 wherein the second substrate
and the second electrically conductive layer are transparent to electromagnetic radiation
having a wavelength in the range of infrared to ultraviolet.
- 27. The multi-layer device of any of aspects 21-26 wherein the multi-layer device
comprises, in succession, the first substrate, the first electrically conductive layer,
the first electrode layer, an ion conducting layer, a second electrode layer, the
second electrically conductive layer and the second substrate.
- 28. The multi-layer device of any of aspects 21-26 wherein the multi-layer device
comprises, in succession, the first substrate, the first electrically conductive layer,
the first electrode layer, the second electrically conductive layer and the second
substrate.
- 29. The multi-layer device of any of aspects 21-26 wherein the multi-layer device
comprises, in succession, the first substrate, the first electrically conductive layer,
the first electrode layer, an ion conducting layer, the second electrically conductive
layer and the second substrate.
- 30. A process for the preparation of a multi-layer device comprising forming a multi-layer
layer structure comprising an electrochromic layer between and in electrical contact
with a first and a second electrically conductive layer, the first and/or the second
electrically conductive layer having a spatially varying sheet resistance, Rs, to the flow of electrical current through the first and/or the second electrically
conductive layer that varies as a function of position in the first and/or the second
electrically conductive layer, respectively, wherein the ratio of the average sheet
resistance in a first region of the first electrically conductive layer circumscribed
by a first convex polygon to the average sheet resistance in a second region of the
first electrically conductive layer circumscribed by a second convex polygon is at
least 2, the first and second regions circumscribed by the first and second convex
polygons, respectively, each comprising at least 25% of the surface area of the first
electrically conductive layer.
- 31. The process of aspect 30 wherein the ratio of the average sheet resistance in
a first region of the first electrically conductive layer, R1avg, to the average sheet resistance in a second region of the first electrically conductive
layer, R2avg, is at least 1.25, the ratio of the average sheet resistance in the second region
of the first electrically conductive layer, R2avg, to the average sheet resistance in a third region of the first electrically conductive
layer, R3avg, is at least 1.25, the ratio of the average sheet resistance in the third region
of the first electrically conductive layer, R3avg, to the average sheet resistance in a fourth region of the first electrically conductive
layer, R4avg, is at least 1.25, wherein the first region is contiguous with the second region,
the second region is contiguous with the third region, the third region is contiguous
with the fourth region, each of the regions is circumscribed by a convex polygon,
and each comprises at least 10% of the surface area of the first electrically conductive
layer.
- 32. The process of aspect 30 or 31 wherein the first electrically conductive layer
has a spatially varying sheet resistance, Rs, that varies as a function of position in the first electrically conductive layer,
a contour map of the sheet resistance, Rs, as a function of position within the first electrically conductive layer contains
a set of isoresistance lines and a set of resistance gradient lines normal to the
isoresistance lines, and the sheet resistance along a gradient line in the set generally
increases, generally decreases, generally increases until it reaches a maximum and
then generally decreases, or generally decreases until it reaches a minimum and then
generally increases.
- 33. The process of any of aspects 30-32 wherein the process comprises depositing the
first electrically conductive layer on a substrate and varying the sheet resistance
of the deposited layer as a function of position in the first electrically conductive
layer.
- 34. The process of any of aspects 30-32 wherein the process comprises depositing a
first electrically conductive layer having a composition or thickness that varies
as a function of position in the first electrically conductive layer.